Temperature compensation in a wireless transfer system
First Claim
1. A resonator for wireless power transfer comprising:
- a conductor forming one or more loops and having an inductance L,a network of capacitors, having a capacitance, C, and a desired electrical parameter, coupled to the conductor, the network having at least one capacitor of a first type with a first temperature profile of the electrical parameter, and the network having at least one capacitor of a second type with a second temperature profile of the electrical parameter.
1 Assignment
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Accused Products

Abstract
Described herein are improved configurations for a resonator for wireless power transfer that includes a conductor forming one or more loops and having an inductance L, a network of capacitors, having a capacitance, C, and a desired electrical parameter, coupled to the conductor, the network having at least one capacitor of a first type with a first temperature profile of the electrical parameter, and the network having at least one capacitor of a second type with a second temperature profile of the electrical parameter.
625 Citations
ADAPTIVE RESONANCE POWER TRANSMITTER | ||
Patent #
US 20120049648A1
Filed 08/30/2011
|
Current Assignee
Samsung Electronics Co. Ltd.
|
Original Assignee
Samsung Electronics Co. Ltd.
|
APPARATUS FOR DETECTING SIGNAL AND WIRELESS POWER TRANSMITTING APPARATUS HAVING THE SAME | ||
Patent #
US 20130162204A1
Filed 12/21/2012
|
Current Assignee
GE Hybrid Technologies LLC
|
Original Assignee
Hanrim Postech Co. Ltd.
|
Energy transfer with vehicles | ||
Patent #
US 8,841,881 B2
Filed 01/28/2011
|
Current Assignee
Bryan Marc Failing
|
Original Assignee
Bryan Marc Failing
|
Wireless energy transfer for medical applications | ||
Patent #
US 8,937,408 B2
Filed 04/20/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Increasing vehicle security | ||
Patent #
US 9,114,719 B1
Filed 05/12/2014
|
Current Assignee
Bryan Marc Failing
|
Original Assignee
Bryan Marc Failing
|
Wireless power transmitting apparatus having signal detecting circuit for detecting transmission signals | ||
Patent #
US 9,246,358 B2
Filed 12/21/2012
|
Current Assignee
GE Hybrid Technologies LLC
|
Original Assignee
Hanrim Postech Co. Ltd.
|
Energy transfer with vehicles | ||
Patent #
US 9,393,878 B1
Filed 09/23/2014
|
Current Assignee
Bryan Marc Failing
|
Original Assignee
Bryan Marc Failing
|
Resonator coil | ||
Patent #
US D769,835 S1
Filed 05/15/2015
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Coil | ||
Patent #
US D770,402 S1
Filed 05/15/2015
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Coil | ||
Patent #
US D770,403 S1
Filed 05/15/2015
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Resonator coil | ||
Patent #
US D770,404 S1
Filed 08/05/2015
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Resonator coil | ||
Patent #
US D773,411 S1
Filed 04/27/2015
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
ENERGY STORAGE SOLUTION FOR AN MRI SYSTEM | ||
Patent #
US 20170102441A1
Filed 10/09/2015
|
Current Assignee
General Electric Company
|
Original Assignee
General Electric Company
|
Environment optimization for space based on presence and activities | ||
Patent #
US 9,642,219 B2
Filed 06/16/2016
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Wireless energy transfer for medical applications | ||
Patent #
US 9,662,161 B2
Filed 12/12/2014
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer for mobile device applications | ||
Patent #
US 9,735,628 B2
Filed 04/16/2015
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Method and system for locating resources and communicating within an enterprise | ||
Patent #
US 9,852,388 B1
Filed 06/10/2016
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Wireless energy transfer for mobile device applications | ||
Patent #
US 9,917,479 B2
Filed 04/16/2015
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Smart workstation method and system | ||
Patent #
US 9,921,726 B1
Filed 06/03/2016
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Resonator coil | ||
Patent #
US D814,432 S1
Filed 02/09/2016
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Space guidance and management system and method | ||
Patent #
US 9,955,318 B1
Filed 06/01/2016
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Wireless charger | ||
Patent #
US D818,434 S1
Filed 06/12/2017
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Resonator coil | ||
Patent #
US D825,503 S1
Filed 06/07/2017
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Environment optimization for space based on presence and activities | ||
Patent #
US 10,057,963 B2
Filed 03/14/2017
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Energy storage solution for an MRI system | ||
Patent #
US 10,067,203 B2
Filed 10/09/2015
|
Current Assignee
General Electric Company
|
Original Assignee
General Electric Company
|
Intelligent multi-mode wireless power system | ||
Patent #
US 10,069,328 B2
Filed 04/05/2017
|
Current Assignee
PowerSphyr Inc.
|
Original Assignee
PowerSphyr Inc.
|
Method and system for locating resources and communicating within an enterprise | ||
Patent #
US 10,121,113 B1
Filed 10/20/2017
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Energy transfer with vehicles | ||
Patent #
US 10,124,691 B1
Filed 09/23/2014
|
Current Assignee
Bryan Marc Failing
|
Original Assignee
Bryan Marc Failing
|
Method and system for locating resources and communicating within an enterprise | ||
Patent #
US 10,161,752 B1
Filed 08/25/2017
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Space guidance and management system and method | ||
Patent #
US 10,225,707 B1
Filed 03/26/2018
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Content amplification system and method | ||
Patent #
US 10,264,213 B1
Filed 12/13/2017
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Method and system for facilitating collaboration sessions | ||
Patent #
US 10,353,664 B2
Filed 06/27/2017
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Intelligent multi-mode wireless power system | ||
Patent #
US 10,411,523 B2
Filed 04/06/2016
|
Current Assignee
PowerSphyr Inc.
|
Original Assignee
PowerSphyr Inc.
|
Microclimate control systems and methods | ||
Patent #
US 10,433,646 B1
Filed 06/27/2017
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Development Inc.
|
Smart workstation method and system | ||
Patent #
US 10,459,611 B1
Filed 02/15/2018
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Multi-mode energy receiver system | ||
Patent #
US 10,483,806 B2
Filed 10/17/2017
|
Current Assignee
PowerSphyr Inc.
|
Original Assignee
PowerSphyr Inc.
|
Intelligent multi-mode wireless power transmitter system | ||
Patent #
US 10,547,211 B2
Filed 10/17/2017
|
Current Assignee
PowerSphyr Inc.
|
Original Assignee
PowerSphyr Inc.
|
Environment optimization for space based on presence and activities | ||
Patent #
US 10,561,006 B2
Filed 07/20/2018
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Powered furniture assembly | ||
Patent #
US 10,614,694 B1
Filed 06/01/2015
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Content amplification system and method | ||
Patent #
US 10,638,090 B1
Filed 01/14/2019
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
Template based content preparation system for use with a plurality of space types | ||
Patent #
US 10,733,371 B1
Filed 06/01/2016
|
Current Assignee
Steelcase Incorporated
|
Original Assignee
Steelcase Incorporated
|
TUNING AND GAIN CONTROL IN ELECTRO-MAGNETIC POWER SYSTEMS | ||
Patent #
US 20110018361A1
Filed 10/01/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q CAPACITIVELY LOADED CONDUCTING LOOPS | ||
Patent #
US 20110043046A1
Filed 12/23/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
High power wireless resonant energy transfer system | ||
Patent #
US 7,880,337 B2
Filed 10/25/2007
|
Current Assignee
Leslie Farkas
|
Original Assignee
Laszlo Farkas
|
WIRELESS DELIVERY OF POWER TO A FIXED-GEOMETRY POWER PART | ||
Patent #
US 20110049998A1
Filed 11/04/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Amplification relay device of electromagnetic wave and a radio electric power conversion apparatus using the above device | ||
Patent #
US 7,885,050 B2
Filed 07/29/2005
|
Current Assignee
Andong National University Industry Academic Cooperation Foundation, JC Protek Company Limited
|
Original Assignee
JC Protek Company Limited
|
RESONATORS FOR WIRELESS POWER TRANSFER | ||
Patent #
US 20110012431A1
Filed 09/10/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20110074347A1
Filed 11/18/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS DESKTOP IT ENVIRONMENT | ||
Patent #
US 20110049996A1
Filed 08/25/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
VEHICLE CHARGER SAFETY SYSTEM AND METHOD | ||
Patent #
US 20110074346A1
Filed 10/06/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20110074218A1
Filed 11/18/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q RESONATORS USING FIELD SHAPING TO IMPROVE K | ||
Patent #
US 20110043049A1
Filed 12/29/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER USING OBJECT POSITIONING FOR LOW LOSS | ||
Patent #
US 20110043048A1
Filed 12/29/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
PACKAGING AND DETAILS OF A WIRELESS POWER DEVICE | ||
Patent #
US 20110025131A1
Filed 10/01/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
IMPLANTABLE PULSE GENERATOR FOR PROVIDING FUNCTIONAL AND/OR THERAPEUTIC STIMULATION OF MUSCLES AND/OR NERVES AND/OR CENTRAL NERVOUS SYSTEM TISSUE | ||
Patent #
US 20110004269A1
Filed 06/28/2010
|
Current Assignee
Medtronic Urinary Solutions Inc.
|
Original Assignee
Medtronic Urinary Solutions Inc.
|
WIRELESS ENERGY TRANSFER USING FIELD SHAPING TO REDUCE LOSS | ||
Patent #
US 20110043047A1
Filed 12/28/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Contactless battery charging apparel | ||
Patent #
US 7,863,859 B2
Filed 06/28/2006
|
Current Assignee
Cynetic Designs Ltd.
|
Original Assignee
Cynetic Designs Ltd.
|
WIRELESS ENERGY TRANSFER RESONATOR THERMAL MANAGEMENT | ||
Patent #
US 20110121920A1
Filed 02/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20110089895A1
Filed 11/18/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
SELECTIVE WIRELESS POWER TRANSFER | ||
Patent #
US 20110115431A1
Filed 08/04/2010
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ENERGY TRANSFER USING REPEATER RESONATORS | ||
Patent #
US 20110095618A1
Filed 04/13/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTIPLE USE WIRELESS POWER SYSTEMS | ||
Patent #
US 20110115303A1
Filed 11/18/2010
|
Current Assignee
Access Business Group International LLC
|
Original Assignee
Access Business Group International LLC
|
Noncontact power transmission system and power transmitting device | ||
Patent #
US 7,923,870 B2
Filed 03/13/2008
|
Current Assignee
Seiko Epson Corporation
|
Original Assignee
Seiko Epson Corporation
|
Inductive power source and charging system | ||
Patent #
US 7,952,322 B2
Filed 01/30/2007
|
Current Assignee
Mojo Mobility Inc.
|
Original Assignee
Mojo Mobility Inc.
|
Foreign Object Detection in Inductive Coupled Devices | ||
Patent #
US 20110128015A1
Filed 10/29/2010
|
Current Assignee
Robert Bosch GmbH
|
Original Assignee
Robert Bosch GmbH
|
Installation | ||
Patent #
US 7,969,045 B2
Filed 05/10/2007
|
Current Assignee
Sew-Eurodrive GmbH Company KG
|
Original Assignee
Sew-Eurodrive GmbH Company KG
|
ADAPTIVE WIRELESS POWER TRANSFER APPARATUS AND METHOD THEREOF | ||
Patent #
US 20110140544A1
Filed 02/18/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
SHORT RANGE EFFICIENT WIRELESS POWER TRANSFER | ||
Patent #
US 20110148219A1
Filed 02/18/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Power receiving device and power transfer system | ||
Patent #
US 7,919,886 B2
Filed 08/29/2008
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Corporation
|
POWER SUPPLY SYSTEM AND METHOD OF CONTROLLING POWER SUPPLY SYSTEM | ||
Patent #
US 20110221278A1
Filed 05/20/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
METHOD AND APPARATUS OF LOAD DETECTION FOR A PLANAR WIRELESS POWER SYSTEM | ||
Patent #
US 20110169339A1
Filed 03/18/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
FLAT, ASYMMETRIC, AND E-FIELD CONFINED WIRELESS POWER TRANSFER APPARATUS AND METHOD THEREOF | ||
Patent #
US 20110198939A1
Filed 03/04/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20110193419A1
Filed 02/28/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESSLY POWERED SPEAKER | ||
Patent #
US 20110181122A1
Filed 04/01/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Wirelessly-chargeable stretch-resistant light-emitting or heat-emitting structure | ||
Patent #
US 20110215086A1
Filed 02/23/2011
|
Current Assignee
WindStream Technology Co. Ltd.
|
Original Assignee
Winharbor Technology Co. Ltd.
|
System to automatically recharge vehicles with batteries | ||
Patent #
US 7,999,506 B1
Filed 04/09/2008
|
Current Assignee
SeventhDigit Corporation
|
Original Assignee
SeventhDigit Corporation
|
ADAPTIVE MATCHING, TUNING, AND POWER TRANSFER OF WIRELESS POWER | ||
Patent #
US 20110227528A1
Filed 05/13/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Energy transferring system and method thereof | ||
Patent #
US 7,994,880 B2
Filed 06/19/2008
|
Current Assignee
Darfon Electronics Corporation
|
Original Assignee
Darfon Electronics Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER SYSTEMS | ||
Patent #
US 20110193416A1
Filed 01/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWER TRANSMISSION FOR PORTABLE WIRELESS POWER CHARGING | ||
Patent #
US 20110227530A1
Filed 05/26/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Wireless non-radiative energy transfer | ||
Patent #
US 8,022,576 B2
Filed 03/31/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
NONCONTACT ELECTRIC POWER RECEIVING DEVICE, NONCONTACT ELECTRIC POWER TRANSMITTING DEVICE, NONCONTACT ELECTRIC POWER FEEDING SYSTEM, AND ELECTRICALLY POWERED VEHICLE | ||
Patent #
US 20110162895A1
Filed 03/18/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Transmitters and receivers for wireless energy transfer | ||
Patent #
US 20110266878A9
Filed 09/16/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
WIRELESS POWER TRANSMISSION SYSTEM | ||
Patent #
US 20110248573A1
Filed 04/06/2011
|
Current Assignee
Panasonic Corporation
|
Original Assignee
Panasonic Corporation
|
WIRELESS POWER TRANSMISSION IN ELECTRIC VEHICLES | ||
Patent #
US 20110254377A1
Filed 04/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Qualcomm Inc.
|
METHODS AND SYSTEMS FOR WIRELESS POWER TRANSMISSION | ||
Patent #
US 20110241618A1
Filed 06/17/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER ANTENNA ALIGNMENT ADJUSTMENT SYSTEM FOR VEHICLES | ||
Patent #
US 20110254503A1
Filed 04/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Qualcomm Inc.
|
Wireless energy transfer using planar capacitively loaded conducting loop resonators | ||
Patent #
US 8,035,255 B2
Filed 11/06/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
OPTIMIZATION OF WIRELESS POWER DEVICES | ||
Patent #
US 20100244576A1
Filed 02/25/2010
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
PHASED ARRAY WIRELESS RESONANT POWER DELIVERY SYSTEM | ||
Patent #
US 20100033021A1
Filed 09/30/2008
|
Current Assignee
Avago Technologies General IP PTE Limited
|
Original Assignee
Broadcom Corporation
|
WIRELESS ENERGY TRANSFER USING VARIABLE SIZE RESONATORS AND SYSTEM MONITORING | ||
Patent #
US 20100164296A1
Filed 12/28/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER WITH FEEDBACK CONTROL FOR LIGHTING APPLICATIONS | ||
Patent #
US 20100201203A1
Filed 02/02/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR REFRIGERATOR APPLICATION | ||
Patent #
US 20100181843A1
Filed 03/11/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWER FOR CHARGEABLE AND CHARGING DEVICES | ||
Patent #
US 20100225272A1
Filed 01/28/2010
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
REDUCED JAMMING BETWEEN RECEIVERS AND WIRELESS POWER TRANSMITTERS | ||
Patent #
US 20100151808A1
Filed 11/05/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS HIGH POWER TRANSFER UNDER REGULATORY CONSTRAINTS | ||
Patent #
US 20100117596A1
Filed 07/06/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Qualcomm Inc.
|
Self-Charging Electric Vehicles and Aircraft, and Wireless Energy Distribution System | ||
Patent #
US 20100231163A1
Filed 09/26/2008
|
Current Assignee
Paradigm Shift Solutions
|
Original Assignee
Governing Dynamics LLC
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20100289449A1
Filed 12/18/2008
|
Current Assignee
Nokia Corporation
|
Original Assignee
Nokia Technologies Oy
|
WIRELESS POWER TRANSFER APPARATUS AND METHOD THEREOF | ||
Patent #
US 20100187913A1
Filed 04/06/2010
|
Current Assignee
Intel Corporation
|
Original Assignee
Intel Corporation
|
EFFICIENCY INDICATOR FOR INCREASING EFFICIENCY OF WIRELESS POWER TRANSFER | ||
Patent #
US 20100201513A1
Filed 10/16/2009
|
Current Assignee
Avago Technologies International Sales Pte Limited
|
Original Assignee
Broadcom Corporation
|
WIRELESS TRANSFER OF INFORMATION USING MAGNETO-ELECTRIC DEVICES | ||
Patent #
US 20100015918A1
Filed 07/17/2009
|
Current Assignee
Ferro Solutions Inc.
|
Original Assignee
Ferro Solutions Inc.
|
METHOD AND APPARATUS FOR SUPPLYING ENERGY TO A MEDICAL DEVICE | ||
Patent #
US 20100234922A1
Filed 10/10/2008
|
Current Assignee
Kirk Promotion Ltd.
|
Original Assignee
Teslux Holding SA
|
WIRELESS POWER TRANSFER SYSTEM AND A LOAD APPARATUS IN THE SAME WIRELESS POWER TRANSFER SYSTEM | ||
Patent #
US 20100164295A1
Filed 11/16/2009
|
Current Assignee
Maxell Ltd.
|
Original Assignee
Hitachi Consumer Electronics Company Limited
|
Security for wireless transfer of electrical power | ||
Patent #
US 20100276995A1
Filed 04/29/2009
|
Current Assignee
Alcatel-Lucent USA Inc.
|
Original Assignee
Alcatel-Lucent USA Inc.
|
WIRELESS POWER TRANSFER FOR FURNISHINGS AND BUILDING ELEMENTS | ||
Patent #
US 20100201202A1
Filed 10/02/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESSLY POWERED SPEAKER | ||
Patent #
US 20100081379A1
Filed 09/25/2009
|
Current Assignee
Intel Corporation
|
Original Assignee
Intel Corporation
|
ELECTRICAL POWERED VEHICLE AND POWER FEEDING DEVICE FOR VEHICLE | ||
Patent #
US 20100225271A1
Filed 09/25/2008
|
Current Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
Original Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
APPLICATIONS OF WIRELESS ENERGY TRANSFER USING COUPLED ANTENNAS | ||
Patent #
US 20100117456A1
Filed 01/15/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER AND DATA TRANSFER FOR ELECTRONIC DEVICES | ||
Patent #
US 20100194335A1
Filed 11/06/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
EFFICIENT NEAR-FIELD WIRELESS ENERGY TRANSFER USING ADIABATIC SYSTEM VARIATIONS | ||
Patent #
US 20100148589A1
Filed 10/01/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
INDUCTIVELY RECHARGEABLE EXTERNAL ENERGY SOURCE, CHARGER, SYSTEM AND METHOD FOR A TRANSCUTANEOUS INDUCTIVE CHARGER FOR AN IMPLANTABLE MEDICAL DEVICE | ||
Patent #
US 20100076524A1
Filed 10/28/2009
|
Current Assignee
Medtronic Incorporated
|
Original Assignee
Medtronic Incorporated
|
SYSTEM FOR ELECTRICAL POWER SUPPLY AND FOR TRANSMITTING DATA WITHOUT ELECTRICAL CONTACT | ||
Patent #
US 20100104031A1
Filed 03/10/2008
|
Current Assignee
Delachaux SA
|
Original Assignee
Delachaux SA
|
RESONANCE-TYPE NON-CONTACT CHARGING APPARATUS | ||
Patent #
US 20100156346A1
Filed 12/23/2009
|
Current Assignee
Toyota Jidoshi Kabushiki Kaisha
|
Original Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha, Kabushiki Kaisha Toyota Jidoshokki
|
INCREASING EFFICIENCY OF WIRELESS POWER TRANSFER | ||
Patent #
US 20100201313A1
Filed 10/16/2009
|
Current Assignee
Avago Technologies International Sales Pte Limited
|
Original Assignee
Broadcom Corporation
|
BIDIRECTIONAL WIRELESS POWER TRANSMISSION | ||
Patent #
US 20100148723A1
Filed 09/01/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS POWER TRANSFER IN PUBLIC PLACES | ||
Patent #
US 20100201201A1
Filed 10/02/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
NONCONTACT ELECTRIC POWER RECEIVING DEVICE, NONCONTACT ELECTRIC POWER TRANSMITTING DEVICE, NONCONTACT ELECTRIC POWER FEEDING SYSTEM, AND ELECTRICALLY POWERED VEHICLE | ||
Patent #
US 20100065352A1
Filed 08/27/2009
|
Current Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
Original Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
WIRELESS POWER TRANSFER FOR CHARGEABLE DEVICES | ||
Patent #
US 20100225270A1
Filed 10/22/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
PACKAGING AND DETAILS OF A WIRELESS POWER DEVICE | ||
Patent #
US 20100327661A1
Filed 09/10/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER USING COUPLED RESONATORS | ||
Patent #
US 20100117455A1
Filed 01/15/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
RETROFITTING WIRELESS POWER AND NEAR-FIELD COMMUNICATION IN ELECTRONIC DEVICES | ||
Patent #
US 20100194334A1
Filed 11/02/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ENERGY TRANSFER SYSTEMS | ||
Patent #
US 20100141042A1
Filed 09/25/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER OVER DISTANCES TO A MOVING DEVICE | ||
Patent #
US 20100187911A1
Filed 12/30/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER TRANSFER WITH LIGHTING | ||
Patent #
US 20100194207A1
Filed 02/04/2010
|
Current Assignee
David S. Graham
|
Original Assignee
David S. Graham
|
Coupling system | ||
Patent #
US 7,825,544 B2
Filed 11/29/2006
|
Current Assignee
Koninklijke Philips N.V.
|
Original Assignee
Koninklijke Philips N.V.
|
RESONATORS AND THEIR COUPLING CHARACTERISTICS FOR WIRELESS POWER TRANSFER VIA MAGNETIC COUPLING | ||
Patent #
US 20100327660A1
Filed 08/26/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
ADAPTIVE MATCHING AND TUNING OF HF WIRELESS POWER TRANSMIT ANTENNA | ||
Patent #
US 20100117454A1
Filed 07/17/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS POWER DISTRIBUTION SYSTEM AND METHOD FOR POWER TOOLS | ||
Patent #
US 20100181964A1
Filed 01/22/2010
|
Current Assignee
Techtronic Power Tools Technology Limited
|
Original Assignee
Techtronic Power Tools Technology Limited
|
SYSTEMS AND METHODS FOR ELECTRIC VEHICLE CHARGING AND POWER MANAGEMENT | ||
Patent #
US 20100017249A1
Filed 07/13/2009
|
Current Assignee
Charge Fusion Technologies LLC
|
Original Assignee
Charge Fusion Technologies LLC
|
Resonator for wireless power transmission | ||
Patent #
US 20100156570A1
Filed 12/17/2009
|
Current Assignee
Samsung Electronics Co. Ltd.
|
Original Assignee
Samsung Electronics Co. Ltd.
|
WIRELESS ENERGY TRANSFER OVER A DISTANCE WITH DEVICES AT VARIABLE DISTANCES | ||
Patent #
US 20100207458A1
Filed 12/16/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Method and Apparatus of Load Detection for a Planar Wireless Power System | ||
Patent #
US 20100066349A1
Filed 09/12/2008
|
Current Assignee
University of Florida Research Foundation Incorporated
|
Original Assignee
University of Florida Research Foundation Incorporated
|
Multilayer structures for magnetic shielding | ||
Patent #
US 7,795,708 B2
Filed 06/02/2006
|
Current Assignee
Honeywell International Inc.
|
Original Assignee
Honeywell International Inc.
|
CONCURRENT WIRELESS POWER TRANSMISSION AND NEAR-FIELD COMMUNICATION | ||
Patent #
US 20100190436A1
Filed 08/25/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ENERGY TRANSFER SYSTEMS | ||
Patent #
US 20100109445A1
Filed 11/06/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Short Range Efficient Wireless Power Transfer | ||
Patent #
US 20100038970A1
Filed 04/21/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Nigel Power LLC
|
Wireless energy transfer | ||
Patent #
US 7,825,543 B2
Filed 03/26/2008
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
APPARATUS FOR DRIVING ARTIFICIAL RETINA USING MEDIUM-RANGE WIRELESS POWER TRANSMISSION TECHNIQUE | ||
Patent #
US 20100094381A1
Filed 06/04/2009
|
Current Assignee
Electronics and Telecommunications Research Institute
|
Original Assignee
Electronics and Telecommunications Research Institute
|
RECEIVE ANTENNA ARRANGEMENT FOR WIRELESS POWER | ||
Patent #
US 20100210233A1
Filed 09/04/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
RESONATOR ARRAYS FOR WIRELESS ENERGY TRANSFER | ||
Patent #
US 20100237709A1
Filed 05/28/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI POWER SOURCED ELECTRIC VEHICLE | ||
Patent #
US 20100109604A1
Filed 05/09/2008
|
Current Assignee
Auckland UniServices Limited
|
Original Assignee
Auckland UniServices Limited
|
WIRELESS ENERGY TRANSFER WITH FREQUENCY HOPPING | ||
Patent #
US 20100171368A1
Filed 12/31/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWER INFRASTRUCTURE | ||
Patent #
US 20100256831A1
Filed 04/03/2009
|
Current Assignee
International Business Machines Corporation
|
Original Assignee
International Business Machines Corporation
|
Apparatus and system for transmitting power wirelessly | ||
Patent #
US 7,843,288 B2
Filed 04/30/2008
|
Current Assignee
Samsung Electronics Co. Ltd., Postech Academy-Industry Foundation
|
Original Assignee
Samsung Electronics Co. Ltd., Postech Academy-Industry Foundation
|
WIRELESS ENERGY TRANSFER BETWEEN A SOURCE AND A VEHICLE | ||
Patent #
US 20100277121A1
Filed 04/29/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q TO MORE THAN ONE DEVICE | ||
Patent #
US 20100127575A1
Filed 12/16/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
ADAPTIVE WIRELESS POWER TRANSFER APPARATUS AND METHOD THEREOF | ||
Patent #
US 20100045114A1
Filed 08/20/2009
|
Current Assignee
Intel Corporation
|
Original Assignee
Intel Corporation
|
WIRELESS POWER TRANSFER SYSTEM | ||
Patent #
US 20100201310A1
Filed 04/10/2009
|
Current Assignee
Avago Technologies General IP PTE Limited
|
Original Assignee
Broadcom Corporation
|
Apparatus for wireless power transmission using high Q low frequency near magnetic field resonator | ||
Patent #
US 20100123530A1
Filed 11/17/2009
|
Current Assignee
Samsung Electronics Co. Ltd.
|
Original Assignee
Samsung Electronics Co. Ltd.
|
ANTENNA SHARING FOR WIRELESSLY POWERED DEVICES | ||
Patent #
US 20100222010A1
Filed 01/28/2010
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
MAGNETIC INDUCTIVE CHARGING WITH LOW FAR FIELDS | ||
Patent #
US 20100244767A1
Filed 03/27/2009
|
Current Assignee
Microsoft Technology Licensing LLC
|
Original Assignee
Microsoft Corporation
|
MAXIMIZING POWER YIELD FROM WIRELESS POWER MAGNETIC RESONATORS | ||
Patent #
US 20100171370A1
Filed 03/18/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER APPARATUS AND WIRELESS POWER-RECEIVING METHOD | ||
Patent #
US 20100244583A1
Filed 03/31/2010
|
Current Assignee
Fujitsu Limited
|
Original Assignee
Fujitsu Limited
|
SYSTEM AND METHOD FOR CHARGING A PLUG-IN ELECTRIC VEHICLE | ||
Patent #
US 20100156355A1
Filed 12/19/2008
|
Current Assignee
GM Global Technology Operations LLC
|
Original Assignee
GM Global Technology Operations Incorporated
|
POWER TRANSMITTING APPARATUS | ||
Patent #
US 20100244839A1
Filed 03/15/2010
|
Current Assignee
Fujitsu Limited
|
Original Assignee
Fujitsu Limited
|
PASSIVE RECEIVERS FOR WIRELESS POWER TRANSMISSION | ||
Patent #
US 20100190435A1
Filed 08/24/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
SPREAD SPECTRUM WIRELESS RESONANT POWER DELIVERY | ||
Patent #
US 20100034238A1
Filed 09/30/2008
|
Current Assignee
Avago Technologies General IP PTE Limited
|
Original Assignee
Broadcom Corporation
|
NON-CONTACT POWER TRANSMISSION DEVICE | ||
Patent #
US 20100052431A1
Filed 09/01/2009
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Corporation
|
NON-CONTACT POWER TRANSMISSION APPARATUS AND METHOD FOR DESIGNING NON-CONTACT POWER TRANSMISSION APPARATUS | ||
Patent #
US 20100115474A1
Filed 11/03/2009
|
Current Assignee
Toyota Industries Corporation
|
Original Assignee
Kabushiki Kaisha Toyota Jidoshokki
|
TRANSMITTERS AND RECEIVERS FOR WIRELESS ENERGY TRANSFER | ||
Patent #
US 20100237708A1
Filed 03/26/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Noncontact Electric Power Transmission System | ||
Patent #
US 20100219696A1
Filed 02/19/2010
|
Current Assignee
Murata Manufacturing Co Limited
|
Original Assignee
TOKO Incorporated
|
PARASITIC DEVICES FOR WIRELESS POWER TRANSFER | ||
Patent #
US 20100277120A1
Filed 04/08/2010
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q SUB-WAVELENGTH RESONATORS | ||
Patent #
US 20100123355A1
Filed 12/16/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q AT HIGH EFFICIENCY | ||
Patent #
US 20100127574A1
Filed 12/16/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER TRANSMISSION SCHEDULING | ||
Patent #
US 20100253281A1
Filed 03/02/2010
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
Power Transfer Apparatus | ||
Patent #
US 20100244582A1
Filed 03/30/2010
|
Current Assignee
Fujitsu Limited
|
Original Assignee
Fujitsu Limited
|
WIRELESS POWERING AND CHARGING STATION | ||
Patent #
US 20100277005A1
Filed 07/16/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
NONCONTACT POWER RECEIVING APPARATUS AND VEHICLE INCLUDING THE SAME | ||
Patent #
US 20100295506A1
Filed 09/19/2008
|
Current Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
Original Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
TRANSMITTERS FOR WIRELESS POWER TRANSMISSION | ||
Patent #
US 20100184371A1
Filed 09/16/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
TRACKING RECEIVER DEVICES WITH WIRELESS POWER SYSTEMS, APPARATUSES, AND METHODS | ||
Patent #
US 20100248622A1
Filed 10/02/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
GLAZING | ||
Patent #
US 20100060077A1
Filed 11/07/2007
|
Current Assignee
Pilkington Automotive Deutschland GmbH
|
Original Assignee
Pilkington Automotive Deutschland GmbH
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q DEVICES AT VARIABLE DISTANCES | ||
Patent #
US 20100123354A1
Filed 12/16/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
IMPEDANCE CHANGE DETECTION IN WIRELESS POWER TRANSMISSION | ||
Patent #
US 20100217553A1
Filed 12/17/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
INTEGRATED WIRELESS RESONANT POWER CHARGING AND COMMUNICATION CHANNEL | ||
Patent #
US 20100036773A1
Filed 09/30/2008
|
Current Assignee
Avago Technologies General IP PTE Limited
|
Original Assignee
Broadcom Corporation
|
FLAT, ASYMMETRIC, AND E-FIELD CONFINED WIRELESS POWER TRANSFER APPARATUS AND METHOD THEREOF | ||
Patent #
US 20100052811A1
Filed 08/20/2009
|
Current Assignee
Intel Corporation
|
Original Assignee
Intel Corporation
|
WIRELESS NON-RADIATIVE ENERGY TRANSFER | ||
Patent #
US 20100102639A1
Filed 09/03/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER ACROSS VARIABLE DISTANCES | ||
Patent #
US 20100102641A1
Filed 12/30/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q SIMILAR RESONANT FREQUENCY RESONATORS | ||
Patent #
US 20100096934A1
Filed 12/23/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER TO A MOVING DEVICE BETWEEN HIGH-Q RESONATORS | ||
Patent #
US 20100102640A1
Filed 12/30/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER TRANSMISSION FOR ELECTRONIC DEVICES | ||
Patent #
US 20100109443A1
Filed 07/27/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ENERGY TRANSFER OVER A DISTANCE AT HIGH EFFICIENCY | ||
Patent #
US 20100127573A1
Filed 12/16/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER TRANSMISSION FOR PORTABLE WIRELESS POWER CHARGING | ||
Patent #
US 20100127660A1
Filed 08/18/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q FROM MORE THAN ONE SOURCE | ||
Patent #
US 20100123353A1
Filed 12/16/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Power supply system and method of controlling power supply system | ||
Patent #
US 20100123452A1
Filed 10/13/2009
|
Current Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
Original Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
WIRELESS ENERGY TRANSFER ACROSS VARIABLE DISTANCES WITH HIGH-Q CAPACITIVELY-LOADED CONDUCTING-WIRE LOOPS | ||
Patent #
US 20100133919A1
Filed 12/30/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Wireless non-radiative energy transfer | ||
Patent #
US 7,741,734 B2
Filed 07/05/2006
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER OVER VARIABLE DISTANCES BETWEEN RESONATORS OF SUBSTANTIALLY SIMILAR RESONANT FREQUENCIES | ||
Patent #
US 20100133918A1
Filed 12/30/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
ADAPTIVE POWER CONTROL FOR WIRELESS CHARGING | ||
Patent #
US 20100181961A1
Filed 11/10/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ENERGY TRANSFER ACROSS A DISTANCE TO A MOVING DEVICE | ||
Patent #
US 20100133920A1
Filed 12/30/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER USING MAGNETIC MATERIALS TO SHAPE FIELD AND REDUCE LOSS | ||
Patent #
US 20100164298A1
Filed 12/28/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER USING CONDUCTING SURFACES TO SHAPE FIELDS AND REDUCE LOSS | ||
Patent #
US 20100164297A1
Filed 12/28/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
HIGH EFFICIENCY AND POWER TRANSFER IN WIRELESS POWER MAGNETIC RESONATORS | ||
Patent #
US 20100181844A1
Filed 03/18/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER TRANSFER FOR VEHICLES | ||
Patent #
US 20100201189A1
Filed 10/02/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS POWER FOR CHARGING DEVICES | ||
Patent #
US 20100194206A1
Filed 11/13/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS POWER CHARGING TIMING AND CHARGING CONTROL | ||
Patent #
US 20100213895A1
Filed 10/30/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
BIOLOGICAL EFFECTS OF MAGNETIC POWER TRANSFER | ||
Patent #
US 20100201205A1
Filed 04/23/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
INDUCED POWER TRANSMISSION CIRCUIT | ||
Patent #
US 20100213770A1
Filed 09/15/2008
|
Current Assignee
Hideo Kikuchi
|
Original Assignee
Hideo Kikuchi
|
NON-CONTACT POWER TRANSMISSION APPARATUS | ||
Patent #
US 20100201316A1
Filed 02/08/2010
|
Current Assignee
Toyota Industries Corporation
|
Original Assignee
Kabushiki Kaisha Toyota Jidoshokki
|
NON-CONTACT POWER TRANSMISSION APPARATUS | ||
Patent #
US 20100201204A1
Filed 02/08/2010
|
Current Assignee
Toyota Industries Corporation
|
Original Assignee
Kabushiki Kaisha Toyota Jidoshokki
|
INCREASING THE Q FACTOR OF A RESONATOR | ||
Patent #
US 20100237707A1
Filed 02/26/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
ELECTRIC POWER SUPPLYING APPARATUS AND ELECTRIC POWER TRANSMITTING SYSTEM USING THE SAME | ||
Patent #
US 20100219695A1
Filed 02/18/2010
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Corporation
|
COIL UNIT, AND POWER TRANSMISSION DEVICE AND POWER RECEPTION DEVICE USING THE COIL UNIT | ||
Patent #
US 20100244579A1
Filed 03/19/2010
|
Current Assignee
Samsung Electronics Co. Ltd.
|
Original Assignee
Seiko Epson Corporation
|
WIRELESS ELECTRIC POWER SUPPLY METHOD AND WIRELESS ELECTRIC POWER SUPPLY APPARATUS | ||
Patent #
US 20100244581A1
Filed 03/29/2010
|
Current Assignee
Fujitsu Limited
|
Original Assignee
Fujitsu Limited
|
WIRELESS ENERGY TRANSFER RESONATOR ENCLOSURES | ||
Patent #
US 20100231340A1
Filed 03/10/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWER SYSTEM AND PROXIMITY EFFECTS | ||
Patent #
US 20100237706A1
Filed 02/19/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER IN LOSSY ENVIRONMENTS | ||
Patent #
US 20100219694A1
Filed 02/13/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
POWER TRANSMMISSION APPARATUS, POWER TRANSMISSION/RECEPTION APPARATUS, AND METHOD OF TRANSMITTING POWER | ||
Patent #
US 20100244578A1
Filed 03/16/2010
|
Current Assignee
Fujitsu Limited
|
Original Assignee
Fujitsu Limited
|
WIRELESS POWER BRIDGE | ||
Patent #
US 20100225175A1
Filed 05/21/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER SUPPLY APPARATUS | ||
Patent #
US 20100244580A1
Filed 03/24/2010
|
Current Assignee
Fujitsu Limited
|
Original Assignee
Fujitsu Limited
|
WIRELESS POWER RANGE INCREASE USING PARASITIC RESONATORS | ||
Patent #
US 20100231053A1
Filed 05/26/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS POWER SUPPLY SYSTEM AND WIRELESS POWER SUPPLY METHOD | ||
Patent #
US 20100244577A1
Filed 03/11/2010
|
Current Assignee
Fujitsu Limited
|
Original Assignee
Fujitsu Limited
|
Method and Apparatus for Automatic Charging of an Electrically Powered Vehicle | ||
Patent #
US 20100235006A1
Filed 04/22/2009
|
Current Assignee
Wendell Brown
|
Original Assignee
Wendell Brown
|
WIRELESS ENERGY TRANSFER CONVERTERS | ||
Patent #
US 20100264747A1
Filed 04/26/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
POWER TRANSMISSION DEVICE, POWER TRANSMISSION METHOD, POWER RECEPTION DEVICE, POWER RECEPTION METHOD, AND POWER TRANSMISSION SYSTEM | ||
Patent #
US 20100259109A1
Filed 04/06/2010
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Corporation
|
WIRELESS POWER TRANSMITTING SYSTEM, POWER RECEIVING STATION, POWER TRANSMITTING STATION, AND RECORDING MEDIUM | ||
Patent #
US 20100264746A1
Filed 03/30/2010
|
Current Assignee
Fujitsu Limited
|
Original Assignee
Fujitsu Limited
|
LONG RANGE LOW FREQUENCY RESONATOR | ||
Patent #
US 20100253152A1
Filed 03/04/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER USING REPEATER RESONATORS | ||
Patent #
US 20100259108A1
Filed 03/10/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
RESONATORS FOR WIRELESS POWER APPLICATIONS | ||
Patent #
US 20100264745A1
Filed 03/18/2010
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
RESONATOR OPTIMIZATIONS FOR WIRELESS ENERGY TRANSFER | ||
Patent #
US 20100259110A1
Filed 04/09/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
PLANAR COIL AND CONTACTLESS ELECTRIC POWER TRANSMISSION DEVICE USING THE SAME | ||
Patent #
US 20100277004A1
Filed 12/24/2008
|
Current Assignee
Panasonic Corporation
|
Original Assignee
Panasonic Corporation
|
MOBILE TERMINALS AND BATTERY PACKS FOR MOBILE TERMINALS | ||
Patent #
US 20100295505A1
Filed 05/24/2010
|
Current Assignee
GE Hybrid Technologies LLC
|
Original Assignee
Hanrim Postech Co. Ltd.
|
ADAPTIVE IMPEDANCE TUNING IN WIRELESS POWER TRANSMISSION | ||
Patent #
US 20100277003A1
Filed 02/25/2010
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
SYSTEMS AND METHODS RELATING TO MULTI-DIMENSIONAL WIRELESS CHARGING | ||
Patent #
US 20100289341A1
Filed 09/25/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
INTEGRATED RESONATOR-SHIELD STRUCTURES | ||
Patent #
US 20100308939A1
Filed 08/20/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Inductively powered secondary assembly | ||
Patent #
US 7,474,058 B2
Filed 11/10/2006
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
INDUCTIVE POWER SUPPLY, REMOTE DEVICE POWERED BY INDUCTIVE POWER SUPPLY AND METHOD FOR OPERATING SAME | ||
Patent #
US 20090010028A1
Filed 09/25/2008
|
Current Assignee
Access Business Group International LLC
|
Original Assignee
Access Business Group International LLC
|
Wireless Energy Transfer Using Coupled Antennas | ||
Patent #
US 20090015075A1
Filed 07/09/2007
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Wireless Power System and Proximity Effects | ||
Patent #
US 20090045772A1
Filed 06/10/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Transmitter head and system for contactless energy transmission | ||
Patent #
US 7,492,247 B2
Filed 02/20/2004
|
Current Assignee
Sew-Eurodrive GmbH Company KG
|
Original Assignee
Sew-Eurodrive GmbH Company KG
|
INCREASING THE Q FACTOR OF A RESONATOR | ||
Patent #
US 20090051224A1
Filed 08/11/2008
|
Current Assignee
Nigel Power LLC
|
Original Assignee
Nigel Power LLC
|
Deployable Antennas for Wireless Power | ||
Patent #
US 20090033564A1
Filed 08/02/2007
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
POWER TRANSMISSION CONTROL DEVICE, POWER TRANSMITTING DEVICE, POWER-TRANSMITTING-SIDE DEVICE, AND NON-CONTACT POWER TRANSMISSION SYSTEM | ||
Patent #
US 20090079387A1
Filed 09/25/2008
|
Current Assignee
Sony Ericsson Mobile Communications Japan Incorporated, Seiko Epson Corporation
|
Original Assignee
Sony Ericsson Mobile Communications Japan Incorporated, Seiko Epson Corporation
|
LONG RANGE LOW FREQUENCY RESONATOR AND MATERIALS | ||
Patent #
US 20090058189A1
Filed 08/11/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
CONTACTLESS POWER SUPPLY | ||
Patent #
US 20090067198A1
Filed 08/28/2008
|
Current Assignee
Powercast Corporation
|
Original Assignee
Michael Thomas Mcelhinny, David Jeffrey Graham, Jesse Frederick Goellner, Alexander Brailovsky
|
High Efficiency and Power Transfer in Wireless Power Magnetic Resonators | ||
Patent #
US 20090072629A1
Filed 09/16/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
VERSATILE APPARATUS AND METHOD FOR ELECTRONIC DEVICES | ||
Patent #
US 20090072782A1
Filed 03/05/2007
|
Current Assignee
Pure Energy Solutions Inc.
|
Original Assignee
Pure Energy Solutions Inc.
|
Antennas for Wireless Power applications | ||
Patent #
US 20090072628A1
Filed 09/14/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Systems and Methods for Wireless Power | ||
Patent #
US 20090058361A1
Filed 06/02/2008
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Maximizing Power Yield from Wireless Power Magnetic Resonators | ||
Patent #
US 20090072627A1
Filed 09/14/2008
|
Current Assignee
Nigel Power LLC
|
Original Assignee
Nigel Power LLC
|
Transmitters and receivers for wireless energy transfer | ||
Patent #
US 20090079268A1
Filed 09/16/2008
|
Current Assignee
Nigel Power LLC
|
Original Assignee
Nigel Power LLC
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20090108679A1
Filed 10/30/2007
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
ATI Technologies ULC
|
Power supply system | ||
Patent #
US 7,514,818 B2
Filed 10/24/2006
|
Current Assignee
Panasonic Electric Works Company Limited
|
Original Assignee
Matsushita Electric Industrial Company Limited
|
SYSTEM AND METHOD FOR INDUCTIVE CHARGING OF PORTABLE DEVICES | ||
Patent #
US 20090096413A1
Filed 05/07/2008
|
Current Assignee
Mojo Mobility Inc.
|
Original Assignee
Mojo Mobility Inc.
|
Power adapter for a remote device | ||
Patent #
US 7,518,267 B2
Filed 10/20/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
SYSTEM, DEVICES, AND METHOD FOR ENERGIZING PASSIVE WIRELESS DATA COMMUNICATION DEVICES | ||
Patent #
US 20090108997A1
Filed 10/31/2007
|
Current Assignee
Intermec IP Corporation
|
Original Assignee
Intermec IP Corporation
|
APPARATUS AND METHOD FOR WIRELESS ENERGY AND/OR DATA TRANSMISSION BETWEEN A SOURCE DEVICE AND AT LEAST ONE TARGET DEVICE | ||
Patent #
US 20090085408A1
Filed 08/29/2008
|
Current Assignee
Maquet GmbH Company KG
|
Original Assignee
Maquet GmbH Company KG
|
PRINTED CIRCUIT BOARD COIL | ||
Patent #
US 20090085706A1
Filed 09/24/2008
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Biological Effects of Magnetic Power Transfer | ||
Patent #
US 20090102292A1
Filed 09/18/2008
|
Current Assignee
Witricity Corporation
|
Original Assignee
Nigel Power LLC
|
Contact-less power transfer | ||
Patent #
US 7,525,283 B2
Filed 02/28/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Wireless Power Range Increase Using Parasitic Antennas | ||
Patent #
US 20090134712A1
Filed 11/26/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Wireless Power Bridge | ||
Patent #
US 20090127937A1
Filed 02/29/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
NON-CONTACT WIRELESS COMMUNICATION APPARATUS, METHOD OF ADJUSTING RESONANCE FREQUENCY OF NON-CONTACT WIRELESS COMMUNICATION ANTENNA, AND MOBILE TERMINAL APPARATUS | ||
Patent #
US 20090146892A1
Filed 11/14/2008
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Ericsson Mobile Communications Japan Incorporated
|
ENERGY TRANSFERRING SYSTEM AND METHOD THEREOF | ||
Patent #
US 20090153273A1
Filed 06/19/2008
|
Current Assignee
Darfon Electronics Corporation
|
Original Assignee
Darfon Electronics Corporation
|
Projector, and mobile device and computer device having the same | ||
Patent #
US 20090161078A1
Filed 12/21/2007
|
Current Assignee
OCULON OPTOELECTRONICS INC.
|
Original Assignee
OCULON OPTOELECTRONICS INC.
|
Antenna arrangement for inductive power transmission and use of the antenna arrangement | ||
Patent #
US 7,545,337 B2
Filed 11/13/2006
|
Current Assignee
Vacuumschmelze GmbH Company KG
|
Original Assignee
Vacuumschmelze GmbH Company KG
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20090160261A1
Filed 12/19/2007
|
Current Assignee
Nokia Corporation
|
Original Assignee
Nokia Corporation
|
Controlling inductive power transfer systems | ||
Patent #
US 7,554,316 B2
Filed 05/11/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Wireless powering and charging station | ||
Patent #
US 20090179502A1
Filed 01/14/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Wireless Power Transfer using Magneto Mechanical Systems | ||
Patent #
US 20090167449A1
Filed 10/13/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
VEHICLE POWER SUPPLY APPARATUS AND VEHICLE WINDOW MEMBER | ||
Patent #
US 20090189458A1
Filed 01/21/2009
|
Current Assignee
Nippon Soken Inc., Ibaraki Toyota Jidosha Kabushiki Kaisha
|
Original Assignee
Ibaraki Toyota Jidosha Kabushiki Kaisha
|
OVEN WITH WIRELESS TEMPERATURE SENSOR FOR USE IN MONITORING FOOD TEMPERATURE | ||
Patent #
US 20090188396A1
Filed 08/05/2008
|
Current Assignee
Premark FEG LLC
|
Original Assignee
Premark FEG LLC
|
INDUCTIVE POWER SUPPLY WITH DUTY CYCLE CONTROL | ||
Patent #
US 20090174263A1
Filed 01/07/2009
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
WIRELESS NON-RADIATIVE ENERGY TRANSFER | ||
Patent #
US 20090195333A1
Filed 03/31/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS NON-RADIATIVE ENERGY TRANSFER | ||
Patent #
US 20090195332A1
Filed 03/31/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Wireless desktop IT environment | ||
Patent #
US 20090212636A1
Filed 01/11/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Antennas and Their Coupling Characteristics for Wireless Power Transfer via Magnetic Coupling | ||
Patent #
US 20090213028A1
Filed 02/26/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Nigel Power LLC
|
APPARATUS, A SYSTEM AND A METHOD FOR ENABLING ELECTROMAGNETIC ENERGY TRANSFER | ||
Patent #
US 20090237194A1
Filed 09/11/2007
|
Current Assignee
Koninklijke Philips N.V.
|
Original Assignee
Koninklijke Philips N.V.
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20090224856A1
Filed 05/08/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Packaging and Details of a Wireless Power device | ||
Patent #
US 20090224609A1
Filed 03/09/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Contactless Battery Charging Apparel | ||
Patent #
US 20090218884A1
Filed 06/28/2006
|
Current Assignee
Cynetic Designs Ltd.
|
Original Assignee
Cynetic Designs Ltd.
|
Ferrite Antennas for Wireless Power Transfer | ||
Patent #
US 20090224608A1
Filed 02/23/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
INDUCTIVE POWER SUPPLY SYSTEM WITH MULTIPLE COIL PRIMARY | ||
Patent #
US 20090230777A1
Filed 03/12/2009
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Power Transmitting Apparatus, Power Transmission Method, Program, and Power Transmission System | ||
Patent #
US 20090271048A1
Filed 04/27/2009
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Corporation
|
POWER TRANSMITTING APPARATUS, POWER RECEIVING APPARATUS, POWER TRANSMISSION METHOD, PROGRAM, AND POWER TRANSMISSION SYSTEM | ||
Patent #
US 20090271047A1
Filed 04/23/2009
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Corporation
|
Tuning and Gain Control in Electro-Magnetic power systems | ||
Patent #
US 20090243394A1
Filed 03/28/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Power Exchange Device, Power Exchange Method, Program, and Power Exchange System | ||
Patent #
US 20090251008A1
Filed 04/01/2009
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Corporation
|
Non-Contact Charger Available Of Wireless Data and Power Transmission, Charging Battery-Pack and Mobile Device Using Non-Contact Charger | ||
Patent #
US 20090261778A1
Filed 10/25/2006
|
Current Assignee
GE Hybrid Technologies LLC
|
Original Assignee
Hanrim Postech Co. Ltd.
|
WIRELESS NON-RADIATIVE ENERGY TRANSFER | ||
Patent #
US 20090267709A1
Filed 03/31/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS NON-RADIATIVE ENERGY TRANSFER | ||
Patent #
US 20090267710A1
Filed 03/31/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Low frequency transcutaneous energy transfer to implanted medical device | ||
Patent #
US 7,599,743 B2
Filed 06/24/2004
|
Current Assignee
Ethicon Endo-Surgery Inc.
|
Original Assignee
Ethicon Endo-Surgery Inc.
|
Packaging and Details of a Wireless Power device | ||
Patent #
US 20090243397A1
Filed 03/04/2009
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Wireless Power Charging System | ||
Patent #
US 20090267558A1
Filed 06/26/2008
|
Current Assignee
GE Hybrid Technologies LLC
|
Original Assignee
Spacon Co. Ltd.
|
WIRELESS CHARGING MODULE AND ELECTRONIC APPARATUS | ||
Patent #
US 20090289595A1
Filed 10/09/2008
|
Current Assignee
Darfon Electronics Corporation
|
Original Assignee
Darfon Electronics Corporation
|
Inductively powered apparatus | ||
Patent #
US 7,615,936 B2
Filed 04/27/2007
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Power Transmission Device, Power Transmission Method, Program, Power Receiving Device and Power Transfer System | ||
Patent #
US 20090281678A1
Filed 05/06/2009
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Corporation
|
REVERSE LINK SIGNALING VIA RECEIVE ANTENNA IMPEDANCE MODULATION | ||
Patent #
US 20090286476A1
Filed 10/10/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
SIGNALING CHARGING IN WIRELESS POWER ENVIRONMENT | ||
Patent #
US 20090286475A1
Filed 10/10/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
METHOD AND APPARATUS FOR AN ENLARGED WIRELESS CHARGING AREA | ||
Patent #
US 20090284218A1
Filed 10/10/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS POWER TRANSFER FOR APPLIANCES AND EQUIPMENTS | ||
Patent #
US 20090284245A1
Filed 11/07/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
TRANSMIT POWER CONTROL FOR A WIRELESS CHARGING SYSTEM | ||
Patent #
US 20090284369A1
Filed 10/10/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
METHOD AND APPARATUS FOR ADAPTIVE TUNING OF WIRELESS POWER TRANSFER | ||
Patent #
US 20090284220A1
Filed 11/06/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ENERGY TRANSFER, INCLUDING INTERFERENCE ENHANCEMENT | ||
Patent #
US 20090284083A1
Filed 05/14/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
RECEIVE ANTENNA FOR WIRELESS POWER TRANSFER | ||
Patent #
US 20090284227A1
Filed 10/10/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
Wireless Delivery of power to a Fixed-Geometry power part | ||
Patent #
US 20090273242A1
Filed 05/05/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
REPEATERS FOR ENHANCEMENT OF WIRELESS POWER TRANSFER | ||
Patent #
US 20090286470A1
Filed 11/06/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
METHOD AND APPARATUS WITH NEGATIVE RESISTANCE IN WIRELESS POWER TRANSFERS | ||
Patent #
US 20090284082A1
Filed 11/06/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
Adaptive inductive power supply | ||
Patent #
US 7,639,514 B2
Filed 03/12/2007
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
CONTROLLING INDUCTIVE POWER TRANSFER SYSTEMS | ||
Patent #
US 20090322158A1
Filed 09/09/2009
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Wireless delivery of power to a mobile powered device | ||
Patent #
US 20090299918A1
Filed 05/28/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Downhole Coils | ||
Patent #
US 20080012569A1
Filed 09/25/2007
|
Current Assignee
Schlumberger Technology Corporation
|
Original Assignee
Schlumberger Technology Corporation
|
Method and apparatus for delivering energy to an electrical or electronic device via a wireless link | ||
Patent #
US 20080014897A1
Filed 01/17/2007
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
WIRELESS ELECTROMAGNETIC PARASITIC POWER TRANSFER | ||
Patent #
US 20080036588A1
Filed 06/25/2007
|
Current Assignee
Securaplane Technologies Inc.
|
Original Assignee
Securaplane Technologies Inc.
|
MRI COMPATIBLE IMPLANTED ELECTRONIC MEDICAL DEVICE WITH POWER AND DATA COMMUNICATION CAPABILITY | ||
Patent #
US 20080051854A1
Filed 08/24/2007
|
Current Assignee
Kenergy Inc.
|
Original Assignee
Kenergy Inc.
|
Flexible Circuit for Downhole Antenna | ||
Patent #
US 20080030415A1
Filed 08/02/2006
|
Current Assignee
Schlumberger Technology Corporation
|
Original Assignee
Schlumberger Technology Corporation
|
Method and apparatus for wireless power transmission | ||
Patent #
US 20080067874A1
Filed 09/14/2007
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
Biothermal power source for implantable devices | ||
Patent #
US 7,340,304 B2
Filed 09/13/2004
|
Current Assignee
Biomed Solutions LLC
|
Original Assignee
Biomed Solutions LLC
|
Inductive power adapter | ||
Patent #
US 7,378,817 B2
Filed 12/12/2003
|
Current Assignee
Microsoft Technology Licensing LLC
|
Original Assignee
Microsoft Corporation
|
Inductive battery charger | ||
Patent #
US 7,375,493 B2
Filed 12/12/2003
|
Current Assignee
Microsoft Technology Licensing LLC
|
Original Assignee
Microsoft Corporation
|
Inductively charged battery pack | ||
Patent #
US 7,375,492 B2
Filed 12/12/2003
|
Current Assignee
Microsoft Technology Licensing LLC
|
Original Assignee
Microsoft Corporation
|
Device for multicentric brain modulation, repair and interface | ||
Patent #
US 20080154331A1
Filed 12/21/2006
|
Current Assignee
University of Pittsburgh of The Commonwealth System of Higher Education
|
Original Assignee
E-Soc, University of Pittsburgh of The Commonwealth System of Higher Education
|
Portable electromagnetic navigation system | ||
Patent #
US 20080132909A1
Filed 12/01/2006
|
Current Assignee
Medtronic Navigation Incorporated
|
Original Assignee
Medtronic Navigation Incorporated
|
Inductively coupled ballast circuit | ||
Patent #
US 7,385,357 B2
Filed 11/28/2006
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
System and method for powering a load | ||
Patent #
US 7,382,636 B2
Filed 10/14/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
INDUCTIVELY COUPLED BALLAST CIRCUIT | ||
Patent #
US 20080191638A1
Filed 02/25/2008
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Transmission Of Power Supply For Robot Applications Between A First Member And A Second Member Arranged Rotatable Relative To One Another | ||
Patent #
US 20080197710A1
Filed 11/30/2005
|
Current Assignee
ABB Research Ltd.
|
Original Assignee
ABB Research Ltd.
|
WIRELESS POWER APPARATUS AND METHODS | ||
Patent #
US 20080211320A1
Filed 01/22/2008
|
Current Assignee
Witricity Corporation
|
Original Assignee
Nigel Power LLC
|
SYSTEM FOR INDUCTIVE POWER TRANSFER | ||
Patent #
US 20080238364A1
Filed 04/02/2007
|
Current Assignee
Visteon Global Technologies Incorporated
|
Original Assignee
Visteon Global Technologies Incorporated
|
Amplification Relay Device of Electromagnetic Wave and a Radio Electric Power Conversion Apparatus Using the Above Device | ||
Patent #
US 20080266748A1
Filed 07/29/2005
|
Current Assignee
Andong National University Industry Academic Cooperation Foundation, JC Protek Company Limited
|
Original Assignee
Andong National University Industry Academic Cooperation Foundation, JC Protek Company Limited
|
No point of contact charging system | ||
Patent #
US 7,443,135 B2
Filed 04/11/2005
|
Current Assignee
GE Hybrid Technologies LLC
|
Original Assignee
Hanrim Postech Co. Ltd.
|
High power wireless resonant energy transfer system | ||
Patent #
US 20080265684A1
Filed 10/25/2007
|
Current Assignee
Leslie Farkas
|
Original Assignee
Laszlo Farkas
|
Kiosk systems and methods | ||
Patent #
US 20080255901A1
Filed 03/26/2008
|
Current Assignee
Ryko Manufacturing Co.
|
Original Assignee
Ryko Manufacturing Co.
|
WIRELESS ENERGY TRANSFER | ||
Patent #
US 20080278264A1
Filed 03/26/2008
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Directional Display Apparatus | ||
Patent #
US 20080273242A1
Filed 05/28/2008
|
Current Assignee
AU Optronics Corporation
|
Original Assignee
Jonathan Harrold, Graham J. Woodgate
|
Tunable Dielectric Resonator Circuit | ||
Patent #
US 20080272860A1
Filed 05/01/2007
|
Current Assignee
Cobham Defense Electronic Systems Corporation
|
Original Assignee
MA Com
|
THERAPY SYSTEM | ||
Patent #
US 20080300657A1
Filed 11/20/2007
|
Current Assignee
ReShape LifeSciences Inc.
|
Original Assignee
ReShape LifeSciences Inc.
|
Resonator structure and method of producing it | ||
Patent #
US 7,466,213 B2
Filed 09/27/2004
|
Current Assignee
Qorvo Inc.
|
Original Assignee
NXP B.V.
|
Wireless battery charging | ||
Patent #
US 7,471,062 B2
Filed 06/12/2002
|
Current Assignee
Koninklijke Philips N.V.
|
Original Assignee
Koninklijke Philips N.V.
|
Portable inductive power station | ||
Patent #
US 7,462,951 B1
Filed 08/11/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Power generation for implantable devices | ||
Patent #
US 20080300660A1
Filed 06/02/2008
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Power transmission system, apparatus and method with communication | ||
Patent #
US 20070010295A1
Filed 07/06/2006
|
Current Assignee
Powercast Llc
|
Original Assignee
Firefly Power Technologies LLC
|
Passive dynamic antenna tuning circuit for a radio frequency identification reader | ||
Patent #
US 20070013483A1
Filed 06/29/2006
|
Current Assignee
Allflex USA Incorporated
|
Original Assignee
Allflex USA Incorporated
|
Implantable device for vital signs monitoring | ||
Patent #
US 20070016089A1
Filed 07/15/2005
|
Current Assignee
Angel Medical Systems Inc., Hi-Tronics Designs Inc.
|
Original Assignee
Angel Medical Systems Inc., Hi-Tronics Designs Inc.
|
Wireless power transmission systems and methods | ||
Patent #
US 20070021140A1
Filed 07/22/2005
|
Current Assignee
Emerson Process Management Power Water Solutions Incorporated
|
Original Assignee
Emerson Process Management Power Water Solutions Incorporated
|
Battery Chargers and Methods for Extended Battery Life | ||
Patent #
US 20070024246A1
Filed 07/27/2006
|
Current Assignee
David Flaugher
|
Original Assignee
David Flaugher
|
Inductively coupled ballast circuit | ||
Patent #
US 7,180,248 B2
Filed 10/22/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Inductive power transfer units having flux shields | ||
Patent #
US 20070064406A1
Filed 09/08/2004
|
Current Assignee
Amway Corporation
|
Original Assignee
Amway Corporation
|
Spatially decoupled twin secondary coils for optimizing transcutaneous energy transfer (TET) power transfer characteristics | ||
Patent #
US 7,191,007 B2
Filed 06/24/2004
|
Current Assignee
Ethicon Endo-Surgery Inc.
|
Original Assignee
Ethicon Endo-Surgery Inc.
|
Resonator system | ||
Patent #
US 7,193,418 B2
Filed 06/13/2005
|
Current Assignee
Bruker Switzerland AG
|
Original Assignee
Bruker Biospin AG
|
CHARGING APPARATUS AND CHARGING SYSTEM | ||
Patent #
US 20070069687A1
Filed 08/09/2006
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Ericsson Mobile Communications Japan Incorporated
|
Radio-frequency (RF) power portal | ||
Patent #
US 20070117596A1
Filed 11/17/2006
|
Current Assignee
Powercast Corporation
|
Original Assignee
Powercast Llc
|
Adaptive inductive power supply | ||
Patent #
US 7,212,414 B2
Filed 10/20/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
RADIO TAG AND SYSTEM | ||
Patent #
US 20070096875A1
Filed 05/22/2006
|
Current Assignee
Visible Assets Incorporated
|
Original Assignee
Visible Assets Incorporated
|
System and method for contact free transfer of power | ||
Patent #
US 20070145830A1
Filed 12/27/2005
|
Current Assignee
Power Science Inc.
|
Original Assignee
MOBILEWISE INC.
|
Power supply system | ||
Patent #
US 7,233,137 B2
Filed 09/23/2004
|
Current Assignee
Sharp Electronics Corporation
|
Original Assignee
Sharp Electronics Corporation
|
ADAPTIVE INDUCTIVE POWER SUPPLY | ||
Patent #
US 20070171681A1
Filed 03/12/2007
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Method for monitoring end of life for battery | ||
Patent #
US 7,251,527 B2
Filed 07/31/2003
|
Current Assignee
Cardiac Pacemakers Incorporated
|
Original Assignee
Cardiac Pacemakers Incorporated
|
Primary units, methods and systems for contact-less power transfer | ||
Patent #
US 7,239,110 B2
Filed 12/01/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Splashpower Limited
|
Portable contact-less power transfer devices and rechargeable batteries | ||
Patent #
US 7,248,017 B2
Filed 11/22/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
SPASHPOWER LIMITED
|
Multi-receiver communication system with distributed aperture antenna | ||
Patent #
US 20070176840A1
Filed 02/06/2003
|
Current Assignee
Hamilton Sundstrand Corporation
|
Original Assignee
Hamilton Sundstrand Corporation
|
INDUCTIVE POWER SOURCE AND CHARGING SYSTEM | ||
Patent #
US 20070182367A1
Filed 01/30/2007
|
Current Assignee
Mojo Mobility Inc.
|
Original Assignee
Mojo Mobility Inc.
|
Method and system for powering an electronic device via a wireless link | ||
Patent #
US 20070178945A1
Filed 04/21/2006
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
Systems and methods of medical monitoring according to patient state | ||
Patent #
US 20070208263A1
Filed 02/27/2007
|
Current Assignee
Angel Medical Systems Inc.
|
Original Assignee
Angel Medical Systems Inc.
|
Wireless non-radiative energy transfer | ||
Patent #
US 20070222542A1
Filed 07/05/2006
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Wireless battery charger via carrier frequency signal | ||
Patent #
US 7,288,918 B2
Filed 03/02/2004
|
Current Assignee
Michael Vincent Distefano
|
Original Assignee
Michael Vincent Distefano
|
Device and Method of Non-Contact Energy Transmission | ||
Patent #
US 20070267918A1
Filed 04/29/2005
|
Current Assignee
Geir Gyland
|
Original Assignee
Geir Gyland
|
Tool for an Industrial Robot | ||
Patent #
US 20070276538A1
Filed 04/06/2004
|
Current Assignee
ABB Research Ltd.
|
Original Assignee
ABB Research Ltd.
|
Adaptive pulse width modulated resonant Class-D converter | ||
Patent #
US 5,986,895 A
Filed 06/05/1998
|
Current Assignee
Astec International Limited
|
Original Assignee
Astec International Limited
|
Tunable ferroelectric resonator arrangement | ||
Patent #
US 7,069,064 B2
Filed 02/20/2004
|
Current Assignee
Telefonaktiebolaget LM Ericsson
|
Original Assignee
Telefonaktiebolaget LM Ericsson
|
Planar resonator for wireless power transfer | ||
Patent #
US 6,960,968 B2
Filed 06/26/2002
|
Current Assignee
Koninklijke Philips N.V.
|
Original Assignee
Koninklijke Philips N.V.
|
Operation in very close coupling of an electromagnetic transponder system | ||
Patent #
US 6,703,921 B1
Filed 04/05/2000
|
Current Assignee
Stmicroelectronics SA
|
Original Assignee
Stmicroelectronics SA
|
Systems and methods for automated resonant circuit tuning | ||
Patent #
US 20060001509A1
Filed 06/29/2005
|
Current Assignee
Stheno Corp.
|
Original Assignee
Phillip R. Gibbs
|
Wireless and powerless sensor and interrogator | ||
Patent #
US 6,988,026 B2
Filed 11/04/2003
|
Current Assignee
American Vehicular Sciences LLC
|
Original Assignee
Automotive Technologies International Incorporated
|
Pulse frequency modulation for induction charge device | ||
Patent #
US 20060022636A1
Filed 07/30/2004
|
Current Assignee
KYE Systems Corporation
|
Original Assignee
KYE Systems Corporation
|
Contact-less power transfer | ||
Patent #
US 20060061323A1
Filed 10/28/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Self-adjusting RF assembly | ||
Patent #
US 20060066443A1
Filed 09/13/2005
|
Current Assignee
Tagsys SA
|
Original Assignee
Tagsys SA
|
Method and apparatus for a wireless power supply | ||
Patent #
US 7,027,311 B2
Filed 10/15/2004
|
Current Assignee
Powercast Corporation
|
Original Assignee
Firefly Power Technologies LLC
|
Feedthrough filter capacitor assembly with internally grounded hermetic insulator | ||
Patent #
US 7,035,076 B1
Filed 08/15/2005
|
Current Assignee
Greatbatch Limited
|
Original Assignee
Greatbatch-Sierra Inc.
|
Contact-less power transfer | ||
Patent #
US 7,042,196 B2
Filed 12/01/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Splashpower Limited
|
Heating system and heater | ||
Patent #
US 20060132045A1
Filed 12/17/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Philips IP Ventures B.V.
|
Method and apparatus for a wireless power supply | ||
Patent #
US 20060164866A1
Filed 02/17/2006
|
Current Assignee
Powercast Corporation
|
Original Assignee
Powercast Corporation
|
Device for brain stimulation using RF energy harvesting | ||
Patent #
US 20060184209A1
Filed 09/02/2005
|
Current Assignee
University of Pittsburgh of The Commonwealth System of Higher Education
|
Original Assignee
University of Pittsburgh of The Commonwealth System of Higher Education
|
Explantation of implantable medical device | ||
Patent #
US 20060184210A1
Filed 04/13/2006
|
Current Assignee
Medtronic Incorporated
|
Original Assignee
Medtronic Incorporated
|
Sensor apparatus management methods and apparatus | ||
Patent #
US 20060181242A1
Filed 03/01/2006
|
Current Assignee
KLA-Tencor Corporation
|
Original Assignee
KLA-Tencor Corporation
|
Energy harvesting circuit | ||
Patent #
US 7,084,605 B2
Filed 10/18/2004
|
Current Assignee
University of Pittsburgh of The Commonwealth System of Higher Education
|
Original Assignee
University Of Pittsburgh
|
Actuator system for use in control of a sheet or web forming process | ||
Patent #
US 20060185809A1
Filed 02/23/2005
|
Current Assignee
ABB Limited
|
Original Assignee
ABB
|
Battery charging assembly for use on a locomotive | ||
Patent #
US 20060214626A1
Filed 03/25/2005
|
Current Assignee
KIM HOTSTART MANUFACTURING COMPANY
|
Original Assignee
KIM HOTSTART MANUFACTURING COMPANY
|
Adapting portable electrical devices to receive power wirelessly | ||
Patent #
US 20060205381A1
Filed 12/16/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Method, apparatus and system for power transmission | ||
Patent #
US 20060199620A1
Filed 02/16/2006
|
Current Assignee
Powercast Llc
|
Original Assignee
Firefly Power Technologies LLC
|
Inductive powering surface for powering portable devices | ||
Patent #
US 20060202665A1
Filed 05/13/2005
|
Current Assignee
Microsoft Technology Licensing LLC
|
Original Assignee
Microsoft Corporation
|
Inductively powered apparatus | ||
Patent #
US 7,126,450 B2
Filed 02/04/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Electric vehicle having multiple-use APU system | ||
Patent #
US 20060219448A1
Filed 03/08/2006
|
Current Assignee
Aptiv Technologies Limited
|
Original Assignee
Delphi Technologies Inc.
|
Inductive coil assembly | ||
Patent #
US 7,116,200 B2
Filed 04/27/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Inductively powered apparatus | ||
Patent #
US 7,118,240 B2
Filed 01/14/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Short-range wireless power transmission and reception | ||
Patent #
US 20060238365A1
Filed 09/12/2005
|
Current Assignee
Elio Vecchione, Conor Keegan
|
Original Assignee
Elio Vecchione, Conor Keegan
|
Biothermal power source for implantable devices | ||
Patent #
US 7,127,293 B2
Filed 03/28/2005
|
Current Assignee
Biomed Solutions LLC
|
Original Assignee
Biomed Solutions LLC
|
Inductive coil assembly | ||
Patent #
US 7,132,918 B2
Filed 10/20/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Power transmission network | ||
Patent #
US 20060270440A1
Filed 05/22/2006
|
Current Assignee
Powercast Corporation
|
Original Assignee
Firefly Power Technologies LLC
|
High Q factor sensor | ||
Patent #
US 7,147,604 B1
Filed 08/07/2002
|
Current Assignee
St. Jude Medical Luxembourg Holdings Ii S.A.R.L.
|
Original Assignee
CardioMEMS Incorporated
|
Powering devices using RF energy harvesting | ||
Patent #
US 20060281435A1
Filed 06/06/2006
|
Current Assignee
Powercast Corporation
|
Original Assignee
Firefly Power Technologies LLC
|
System, method and apparatus for contact-less battery charging with dynamic control | ||
Patent #
US 6,844,702 B2
Filed 05/16/2002
|
Current Assignee
Koninklijke Philips N.V.
|
Original Assignee
Koninklijke Philips N.V.
|
Method of rendering a mechanical heart valve non-thrombogenic with an electrical device | ||
Patent #
US 20050021134A1
Filed 06/30/2004
|
Current Assignee
JS Vascular Inc.
|
Original Assignee
JS Vascular Inc.
|
Vehicle interface | ||
Patent #
US 20050007067A1
Filed 06/18/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Multi-frequency piezoelectric energy harvester | ||
Patent #
US 6,858,970 B2
Filed 10/21/2002
|
Current Assignee
The Boeing Co.
|
Original Assignee
The Boeing Co.
|
Temperature regulated implant | ||
Patent #
US 20050033382A1
Filed 08/04/2004
|
Current Assignee
Cochlear Limited
|
Original Assignee
Peter Single
|
Energy transfer amplification for intrabody devices | ||
Patent #
US 20050027192A1
Filed 07/29/2003
|
Current Assignee
Biosense Webster Incorporated
|
Original Assignee
Biosense Webster Incorporated
|
Energy harvesting circuits and associated methods | ||
Patent #
US 6,856,291 B2
Filed 07/21/2003
|
Current Assignee
University Of Pittsburgh
|
Original Assignee
University of Pittsburgh of The Commonwealth System of Higher Education
|
Method and apparatus for efficient power/data transmission | ||
Patent #
US 20050085873A1
Filed 10/14/2004
|
Current Assignee
Alfred E. Mann Foundation For Scientific Research
|
Original Assignee
Alfred E. Mann Foundation For Scientific Research
|
Inductively coupled ballast circuit | ||
Patent #
US 20050093475A1
Filed 10/22/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Method and apparatus for a wireless power supply | ||
Patent #
US 20050104453A1
Filed 10/15/2004
|
Current Assignee
Powercast Corporation
|
Original Assignee
Firefly Power Technologies LLC
|
Method of manufacturing a lamp assembly | ||
Patent #
US 20050116650A1
Filed 10/29/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Contact-less power transfer | ||
Patent #
US 20050140482A1
Filed 12/01/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Lily Ka-Lai Cheng, James Westwood Hay, Pilgrim Giles William Beart
|
Contact-less power transfer | ||
Patent #
US 6,906,495 B2
Filed 12/20/2002
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Splashpower Limited
|
Opportunistic power supply charge system for portable unit | ||
Patent #
US 20050127866A1
Filed 12/11/2003
|
Current Assignee
Symbol Technologies LLC
|
Original Assignee
Symbol Technologies Inc.
|
Inductively powered apparatus | ||
Patent #
US 20050127849A1
Filed 01/14/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Christopher Houghton, Stephen J. Mcphilliamy, David W. Baarman
|
Inductively powered apparatus | ||
Patent #
US 20050122059A1
Filed 01/14/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Christopher Houghton, Stephen J. Mcphilliamy, David W. Baarman
|
Inductively powered apparatus | ||
Patent #
US 20050122058A1
Filed 01/14/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Christopher Houghton, Stephen J. Mcphilliamy, David W. Baarman
|
Inductively powered apparatus | ||
Patent #
US 20050127850A1
Filed 01/14/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Christopher Houghton, Stephen J. Mcphilliamy, David W. Baarman
|
Inductively powered lamp assembly | ||
Patent #
US 6,917,163 B2
Filed 02/18/2004
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Mach-Zehnder interferometer using photonic band gap crystals | ||
Patent #
US 6,917,431 B2
Filed 05/15/2002
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Charging apparatus by non-contact dielectric feeding | ||
Patent #
US 20050156560A1
Filed 04/04/2003
|
Current Assignee
ALPS Electric Company Limited
|
Original Assignee
ALPS Electric Company Limited
|
Magnetic field production system, and configuration for wire-free supply of a large number of sensors and/or actuators using a magnetic field production system | ||
Patent #
US 6,937,130 B2
Filed 09/16/2002
|
Current Assignee
ABB Research Ltd.
|
Original Assignee
ABB Research Ltd.
|
Method and apparatus of using magnetic material with residual magnetization in transient electromagnetic measurement | ||
Patent #
US 20050189945A1
Filed 01/18/2005
|
Current Assignee
Baker Hughes Incorporated
|
Original Assignee
Baker Hughes Incorporated
|
Wireless battery charger via carrier frequency signal | ||
Patent #
US 20050194926A1
Filed 03/02/2004
|
Current Assignee
Michael Vincent Di Stefano
|
Original Assignee
Michael Vincent Di Stefano
|
Non-contact pumping of light emitters via non-radiative energy transfer | ||
Patent #
US 20050253152A1
Filed 05/11/2004
|
Current Assignee
Los Alamos National Security LLC
|
Original Assignee
Los Alamos National Security LLC
|
Subcutaneously implantable power supply | ||
Patent #
US 6,961,619 B2
Filed 07/08/2002
|
Current Assignee
Don E. Casey
|
Original Assignee
Don E. Casey
|
Charging of devices by microwave power beaming | ||
Patent #
US 6,967,462 B1
Filed 06/05/2003
|
Current Assignee
NasaGlenn Research Center
|
Original Assignee
NasaGlenn Research Center
|
Transcutaneous energy transfer primary coil with a high aspect ferrite core | ||
Patent #
US 20050288742A1
Filed 06/24/2004
|
Current Assignee
Ethicon Endo-Surgery Inc.
|
Original Assignee
Ethicon Endo-Surgery Inc.
|
Medical implant having closed loop transcutaneous energy transfer (TET) power transfer regulation circuitry | ||
Patent #
US 20050288739A1
Filed 06/24/2004
|
Current Assignee
Ethicon Endo-Surgery Inc.
|
Original Assignee
Ethicon Incorporated
|
Low frequency transcutaneous energy transfer to implanted medical device | ||
Patent #
US 20050288741A1
Filed 06/24/2004
|
Current Assignee
Ethicon Endo-Surgery Inc.
|
Original Assignee
Ethicon Endo-Surgery Inc.
|
Inductive coil assembly | ||
Patent #
US 6,975,198 B2
Filed 04/27/2005
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Low frequency transcutaneous telemetry to implanted medical device | ||
Patent #
US 20050288740A1
Filed 06/24/2004
|
Current Assignee
Ethicon Endo-Surgery Inc.
|
Original Assignee
Ethicon Endo-Surgery Inc.
|
Planar resonator for wireless power transfer | ||
Patent #
US 20040000974A1
Filed 06/26/2002
|
Current Assignee
Koninklijke Philips N.V.
|
Original Assignee
Koninklijke Philips N.V.
|
Radio frequency identification system for a fluid treatment system | ||
Patent #
US 6,673,250 B2
Filed 06/18/2002
|
Current Assignee
Access Business Group International LLC
|
Original Assignee
Access Business Group International LLC
|
Oscillator module incorporating looped-stub resonator | ||
Patent #
US 20040100338A1
Filed 11/13/2003
|
Current Assignee
Microsemi Corporation
|
Original Assignee
Phasor Technologies Corporation
|
Inductively powered lamp assembly | ||
Patent #
US 6,731,071 B2
Filed 04/26/2002
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Antenna with near-field radiation control | ||
Patent #
US 20040113847A1
Filed 12/12/2002
|
Current Assignee
Blackberry Limited
|
Original Assignee
Blackberry Limited
|
System for a machine having a large number of proximity sensors, as well as a proximity sensor, and a primary winding for this purpose | ||
Patent #
US 6,749,119 B2
Filed 12/11/2001
|
Current Assignee
ABB Research Ltd.
|
Original Assignee
ABB Research Ltd.
|
Adaptive inductive power supply with communication | ||
Patent #
US 20040130915A1
Filed 10/20/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Adaptive inductive power supply | ||
Patent #
US 20040130916A1
Filed 10/20/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Remote power recharge for electronic equipment | ||
Patent #
US 20040142733A1
Filed 12/29/2003
|
Current Assignee
Ronald J. Parise
|
Original Assignee
Ronald J. Parise
|
Adapter | ||
Patent #
US 20040150934A1
Filed 10/20/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Transmission of information from an implanted medical device | ||
Patent #
US 6,772,011 B2
Filed 08/20/2002
|
Current Assignee
TC1 LLC
|
Original Assignee
Thoratec LLC
|
System and method for wireless electrical power transmission | ||
Patent #
US 6,798,716 B1
Filed 06/19/2003
|
Current Assignee
BC SYSTEMS INC.
|
Original Assignee
BC SYSTEMS INC.
|
System and method for inductive charging a wireless mouse | ||
Patent #
US 20040189246A1
Filed 12/16/2003
|
Current Assignee
SelfCHARGE Inc.
|
Original Assignee
SelfCHARGE Inc.
|
Starter assembly for a gas discharge lamp | ||
Patent #
US 6,806,649 B2
Filed 02/18/2003
|
Current Assignee
Access Business Group International LLC
|
Original Assignee
Access Business Group International LLC
|
Charging system for robot | ||
Patent #
US 20040201361A1
Filed 11/14/2003
|
Current Assignee
Samsung Electronics Co. Ltd.
|
Original Assignee
Samsung Electronics Co. Ltd.
|
Inductively powered lamp assembly | ||
Patent #
US 6,812,645 B2
Filed 06/05/2003
|
Current Assignee
Access Business Group International LLC
|
Original Assignee
Access Business Group International LLC
|
Communication system | ||
Patent #
US 20040233043A1
Filed 11/13/2003
|
Current Assignee
Hitachi America Limited
|
Original Assignee
Hitachi America Limited
|
Starter assembly for a gas discharge lamp | ||
Patent #
US 20040222751A1
Filed 05/20/2004
|
Current Assignee
Access Business Group International LLC
|
Original Assignee
Scott A. Mollema, Roy W. Kuennen, David W. Baarman
|
Inductive coil assembly | ||
Patent #
US 20040232845A1
Filed 10/20/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Inductively coupled ballast circuit | ||
Patent #
US 6,825,620 B2
Filed 09/18/2002
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Wireless power transmission | ||
Patent #
US 20040227057A1
Filed 04/07/2004
|
Current Assignee
AILOCOM OY
|
Original Assignee
AILOCOM OY
|
Sensor apparatus management methods and apparatus | ||
Patent #
US 20040267501A1
Filed 07/10/2004
|
Current Assignee
KLA-Tencor Corporation
|
Original Assignee
KLA-Tencor Corporation
|
Method of manufacturing a lamp assembly | ||
Patent #
US 6,831,417 B2
Filed 06/05/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Method and apparatus for supplying contactless power | ||
Patent #
US 6,515,878 B1
Filed 08/07/1998
|
Current Assignee
MEINS-SINSLEY PARTNERSHIP
|
Original Assignee
MEINS-SINSLEY PARTNERSHIP
|
Proximity sensor | ||
Patent #
US 20030038641A1
Filed 09/03/2002
|
Current Assignee
ABB Research Ltd.
|
Original Assignee
ABB Research Ltd.
|
Vehicle slide door power supply apparatus and method of supplying power to vehicle slide door | ||
Patent #
US 6,535,133 B2
Filed 11/15/2001
|
Current Assignee
Yazaki Corporation
|
Original Assignee
Yazaki Corporation
|
Resonant frequency tracking system and method for use in a radio frequency (RF) power supply | ||
Patent #
US 20030071034A1
Filed 11/25/2002
|
Current Assignee
Ambrell Corporation
|
Original Assignee
Daniel J. Lincoln, Gary A. Schwenck, Leslie L. Thompson
|
Magnetic field production system, and configuration for wire-free supply of a large number of sensors and/or actuators using a magnetic field production system | ||
Patent #
US 20030062794A1
Filed 09/16/2002
|
Current Assignee
ABB Research Ltd.
|
Original Assignee
ABB Research Ltd.
|
Configuration for producing electrical power from a magnetic field | ||
Patent #
US 20030062980A1
Filed 09/09/2002
|
Current Assignee
ABB Research Ltd.
|
Original Assignee
ABB Research Ltd.
|
High purity fine metal powders and methods to produce such powders | ||
Patent #
US 20030126948A1
Filed 12/10/2002
|
Current Assignee
PPG Industries Ohio Incorporated
|
Original Assignee
NanoProducts Corporation
|
Post-processed nanoscale powders and method for such post-processing | ||
Patent #
US 20030124050A1
Filed 03/29/2002
|
Current Assignee
PPG Industries Ohio Incorporated
|
Original Assignee
NANOPRODUCT CORPORATION
|
System for wirelessly supplying a large number of actuators of a machine with electrical power | ||
Patent #
US 6,597,076 B2
Filed 12/11/2001
|
Current Assignee
ABB Patent GmbH
|
Original Assignee
ABB Patent GmbH
|
System for the detection of cardiac events | ||
Patent #
US 6,609,023 B1
Filed 09/20/2002
|
Current Assignee
Angel Medical Systems Inc.
|
Original Assignee
Angel Medical Systems Inc.
|
Apparatus for energizing a remote station and related method | ||
Patent #
US 20030199778A1
Filed 06/11/2003
|
Current Assignee
University Of Pittsburgh
|
Original Assignee
Leonid Mats, Carl Taylor, Minhong Mi, Dmitry Gorodetsky, Lorenz Neureuter, Marlin Mickle, Chad Emahizer
|
Charge storage device | ||
Patent #
US 6,631,072 B1
Filed 08/24/2001
|
Current Assignee
Cap-Xx Ltd.
|
Original Assignee
Energy Storage Systems Inc.
|
Inductively powered apparatus | ||
Patent #
US 20030214255A1
Filed 02/04/2003
|
Current Assignee
Philips IP Ventures B.V.
|
Original Assignee
Access Business Group International LLC
|
Wireless power transmission system with increased output voltage | ||
Patent #
US 6,664,770 B1
Filed 10/10/2001
|
Current Assignee
IQ-MOBIL ELECTRONICS GMBH.
|
Original Assignee
IQ- MOBIL GMBH
|
Low-power, high-modulation-index amplifier for use in battery-powered device | ||
Patent #
US 20020032471A1
Filed 08/31/2001
|
Current Assignee
Boston Scientific Neuromodulation Corporation
|
Original Assignee
Advanced Bionics Corporation
|
System for wirelessly supplying a large number of actuators of a machine with electrical power | ||
Patent #
US 20020118004A1
Filed 12/11/2001
|
Current Assignee
ABB Patent GmbH
|
Original Assignee
ABB Patent GmbH
|
Water treatment system with an inductively coupled ballast | ||
Patent #
US 6,436,299 B1
Filed 06/12/2000
|
Current Assignee
Access Business Group International LLC
|
Original Assignee
Amway Corporation
|
System for a machine having a large number of proximity sensors, as well as a proximity sensor, and a primary winding for this purpose | ||
Patent #
US 20020105343A1
Filed 12/11/2001
|
Current Assignee
ABB Research Ltd.
|
Original Assignee
ABB Research Ltd.
|
Food intake restriction with wireless energy transfer | ||
Patent #
US 6,450,946 B1
Filed 02/11/2000
|
Current Assignee
Obtech Medical AG
|
Original Assignee
Obtech Medical AG
|
High quality-factor tunable resonator | ||
Patent #
US 6,452,465 B1
Filed 06/27/2000
|
Current Assignee
M-SQUARED FILTERS L.L.C.
|
Original Assignee
M-SQUARED FILTERS LLC
|
Inductive coupling system with capacitive parallel compensation of the mutual self-inductance between the primary and the secondary windings | ||
Patent #
US 20020130642A1
Filed 02/27/2002
|
Current Assignee
Koninklijke Philips N.V.
|
Original Assignee
Koninklijke Philips N.V.
|
Detection of the distance between an electromagnetic transponder and a terminal | ||
Patent #
US 6,473,028 B1
Filed 04/05/2000
|
Current Assignee
Stmicroelectronics SA
|
Original Assignee
Stmicroelectronics SA
|
Control of inductive power transfer pickups | ||
Patent #
US 6,483,202 B1
Filed 07/24/2000
|
Current Assignee
Auckland UniServices Limited
|
Original Assignee
Auckland UniServices Limited
|
Rechargeable power supply system and method of protection against abnormal charging | ||
Patent #
US 20020167294A1
Filed 03/20/2002
|
Current Assignee
Acer Inc.
|
Original Assignee
International Business Machines Corporation
|
Contactless battery charger with wireless control link | ||
Patent #
US 6,184,651 B1
Filed 03/20/2000
|
Current Assignee
Google Technology Holdings LLC
|
Original Assignee
Motorola Inc.
|
Miniature milliwatt electric power generator | ||
Patent #
US 6,207,887 B1
Filed 07/07/1999
|
Current Assignee
HI-Z Technology Inc.
|
Original Assignee
HI-Z Technology Inc.
|
Electrosurgical generator | ||
Patent #
US 6,238,387 B1
Filed 11/16/1998
|
Current Assignee
Microline Surgical Inc.
|
Original Assignee
Team Medical LLC
|
Integrated tunable high efficiency power amplifier | ||
Patent #
US 6,232,841 B1
Filed 07/01/1999
|
Current Assignee
OL Security LLC
|
Original Assignee
Rockwell Science Center LLC
|
Rechargeable hybrid battery/supercapacitor system | ||
Patent #
US 6,252,762 B1
Filed 04/21/1999
|
Current Assignee
Rutgers University
|
Original Assignee
Telcordia Technologies Incorporated
|
Method for discriminating between used and unused gas generators for air bags during car scrapping process | ||
Patent #
US 6,012,659 A
Filed 09/12/1997
|
Current Assignee
Daicel Chemical Industries Limited, Toyota Jidosha Kabushiki Kaisha
|
Original Assignee
Daicel Chemical Industries Limited, Toyota Jidosha Kabushiki Kaisha
|
Adaptive brain stimulation method and system | ||
Patent #
US 6,066,163 A
Filed 02/02/1996
|
Current Assignee
Michael Sasha John
|
Original Assignee
Michael Sasha John
|
Implantable medical device using audible sound communication to provide warnings | ||
Patent #
US 6,067,473 A
Filed 03/31/1999
|
Current Assignee
Medtronic Incorporated
|
Original Assignee
Medtronic Incorporated
|
Battery monitoring apparatus and method for programmers of cardiac stimulating devices | ||
Patent #
US 6,108,579 A
Filed 04/11/1997
|
Current Assignee
Pacesetter Incorporated
|
Original Assignee
Pacesetter Incorporated
|
Method and apparatus for wireless powering and recharging | ||
Patent #
US 6,127,799 A
Filed 05/14/1999
|
Current Assignee
Raytheon BBN Technlogies Corp.
|
Original Assignee
GTE Internetworking Incorporated
|
Non-contact power distribution system | ||
Patent #
US 5,898,579 A
Filed 11/24/1997
|
Current Assignee
Auckland UniServices Limited, Daifuku Company Limited
|
Original Assignee
Auckland UniServices Limited, Daifuku Company Limited
|
Inductive battery charger | ||
Patent #
US 5,903,134 A
Filed 05/19/1998
|
Current Assignee
Tdk-Lambda Corporation
|
Original Assignee
Nippon Electric Industry Company Limited
|
Noncontact power transmitting apparatus | ||
Patent #
US 5,923,544 A
Filed 07/21/1997
|
Current Assignee
TDK Corporation
|
Original Assignee
TDK Corporation
|
Method and apparatus for controlling country specific frequency allocation | ||
Patent #
US 5,940,509 A
Filed 11/18/1997
|
Current Assignee
Avago Technologies General IP PTE Limited
|
Original Assignee
Intermec IP Corporation
|
Implantable cardioverter defibrillator having a smaller mass | ||
Patent #
US 5,957,956 A
Filed 11/03/1997
|
Current Assignee
Ela Medical S.A.
|
Original Assignee
Angeion Corporation
|
Carbon supercapacitor electrode materials | ||
Patent #
US 5,993,996 A
Filed 09/16/1997
|
Current Assignee
INORGANIC SPECIALISTS INC.
|
Original Assignee
INORGANIC SPECIALISTS INC.
|
Methods and systems for introducing electromagnetic radiation into photonic crystals | ||
Patent #
US 5,999,308 A
Filed 04/01/1998
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
H-field electromagnetic heating system for fusion bonding | ||
Patent #
US 5,710,413 A
Filed 03/29/1995
|
Current Assignee
3M Company
|
Original Assignee
3M Company
|
Nanostructure multilayer dielectric materials for capacitors and insulators | ||
Patent #
US 5,742,471 A
Filed 11/25/1996
|
Current Assignee
Lawrence Livermore National Security LLC
|
Original Assignee
Regents of the University of California
|
Connection system and connection method for an electric automotive vehicle | ||
Patent #
US 5,821,731 A
Filed 01/30/1997
|
Current Assignee
Sumitomo Wiring Systems Limited
|
Original Assignee
Sumitomo Wiring Systems Limited
|
Armature induction charging of moving electric vehicle batteries | ||
Patent #
US 5,821,728 A
Filed 07/22/1996
|
Current Assignee
Stanley A. Tollison
|
Original Assignee
Stanley A. Tollison
|
Method and apparatus for the suppression of far-field interference signals for implantable device data transmission systems | ||
Patent #
US 5,630,835 A
Filed 07/24/1995
|
Current Assignee
SIRROM CAPITAL CORPORATION
|
Original Assignee
CARDIAC CONTROL SYSTEMS INC.
|
Implantable stimulation device having means for optimizing current drain | ||
Patent #
US 5,697,956 A
Filed 06/02/1995
|
Current Assignee
Pacesetter Incorporated
|
Original Assignee
Pacesetter Incorporated
|
Inductive coupler for electric vehicle charger | ||
Patent #
US 5,703,461 A
Filed 06/27/1996
|
Current Assignee
KABUSHIKI KAIHSA TOYODA JIDOSHOKKI SEISAKUSHO
|
Original Assignee
Kabushiki Kaisha Toyoda Jidoshokki Seisakusho
|
Oscillator-shuttle-circuit (OSC) networks for conditioning energy in higher-order symmetry algebraic topological forms and RF phase conjugation | ||
Patent #
US 5,493,691 A
Filed 12/23/1993
|
Current Assignee
BARRETT HOLDING LLC
|
Original Assignee
Terence W. Barrett
|
Inductive power pick-up coils | ||
Patent #
US 5,528,113 A
Filed 10/21/1994
|
Current Assignee
Auckland UniServices Limited
|
Original Assignee
Auckland UniServices Limited
|
Pacemaker with improved shelf storage capacity | ||
Patent #
US 5,522,856 A
Filed 09/20/1994
|
Current Assignee
VITATRON MEDICAL B.V.
|
Original Assignee
VITATRON MEDICAL B.V.
|
Induction charging apparatus | ||
Patent #
US 5,550,452 A
Filed 07/22/1994
|
Current Assignee
Kyushu Hitachi Maxell Ltd., Nintendo Company Limited
|
Original Assignee
Kyushu Hitachi Maxell Ltd., Nintendo Company Limited
|
Thermoelectric method and apparatus for charging superconducting magnets | ||
Patent #
US 5,565,763 A
Filed 11/19/1993
|
Current Assignee
General Atomics Inc.
|
Original Assignee
Lockheed Martin Corporation
|
Cooled secondary coils of electric automobile charging transformer | ||
Patent #
US 5,408,209 A
Filed 11/02/1993
|
Current Assignee
GM Global Technology Operations LLC
|
Original Assignee
Hughes Aircraft Company
|
Wireless communications using near field coupling | ||
Patent #
US 5,437,057 A
Filed 12/03/1992
|
Current Assignee
Xerox Corporation
|
Original Assignee
Xerox Corporation
|
Power connection scheme | ||
Patent #
US 5,455,467 A
Filed 03/02/1994
|
Current Assignee
Apple Computer Incorporated
|
Original Assignee
Apple Computer Incorporated
|
High speed read/write AVI system | ||
Patent #
US 5,287,112 A
Filed 04/14/1993
|
Current Assignee
Texas Instruments Inc.
|
Original Assignee
Texas Instruments Inc.
|
Contactless battery charging system | ||
Patent #
US 5,341,083 A
Filed 10/20/1992
|
Current Assignee
Electric Power Research Institute
|
Original Assignee
Electric Power Research Institute Incorporated
|
System for charging a rechargeable battery of a portable unit in a rack | ||
Patent #
US 5,367,242 A
Filed 09/18/1992
|
Current Assignee
Ascom Tateco AB
|
Original Assignee
Ericsson Messaging Systems Incorporated
|
Separable inductive coupler | ||
Patent #
US 5,216,402 A
Filed 01/22/1992
|
Current Assignee
General Motors Corporation
|
Original Assignee
Hughes Aircraft Company
|
Non-contact data and power connector for computer based modules | ||
Patent #
US 5,229,652 A
Filed 04/20/1992
|
Current Assignee
Wayne E. Hough
|
Original Assignee
Wayne E. Hough
|
Dual feedback control for a high-efficiency class-d power amplifier circuit | ||
Patent #
US 5,118,997 A
Filed 08/16/1991
|
Current Assignee
General Electric Company
|
Original Assignee
General Electric Company
|
Magnetic induction mine arming, disarming and simulation system | ||
Patent #
US 5,027,709 A
Filed 11/13/1990
|
Current Assignee
Glenn B. Slagle
|
Original Assignee
Glenn B. Slagle
|
Transponder arrangement | ||
Patent #
US 5,053,774 A
Filed 02/13/1991
|
Current Assignee
Texas Instruments Deutschland Gesellschaft Mit BeschrNkter Haftung
|
Original Assignee
Texas Instruments Deutschland Gesellschaft Mit BeschrNkter Haftung
|
Electric power transmitting device with inductive coupling | ||
Patent #
US 5,070,293 A
Filed 03/02/1990
|
Current Assignee
Nippon Soken Inc., Nippondenso Co. Ltd.
|
Original Assignee
Nippon Soken Inc., Nippondenso Co. Ltd.
|
Variable mutual transductance tuned antenna | ||
Patent #
US 4,280,129 A
Filed 09/10/1979
|
Current Assignee
WELLS FAMILY CORPORATION THE
|
Original Assignee
Donald H. Wells
|
RF beam center location method and apparatus for power transmission system | ||
Patent #
US 4,088,999 A
Filed 05/21/1976
|
Current Assignee
Fletcher James C Administrator of The National Aeronautics and Space Administration With Respect To An Invention of, Richard M. Dickinson
|
Original Assignee
Fletcher James C Administrator of The National Aeronautics and Space Administration With Respect To An Invention of, Richard M. Dickinson
|
Thermoelectric voltage generator | ||
Patent #
US 4,095,998 A
Filed 09/30/1976
|
Current Assignee
The United States Of America As Represented By The Secretary Of The Army
|
Original Assignee
The United States Of America As Represented By The Secretary Of The Army
|
Wireless energy transfer, including interference enhancement | ||
Patent #
US 8,076,801 B2
Filed 05/14/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Wireless Power Harvesting and Transmission with Heterogeneous Signals. | ||
Patent #
US 20120007441A1
Filed 08/29/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless non-radiative energy transfer | ||
Patent #
US 8,076,800 B2
Filed 03/31/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Wireless energy transfer | ||
Patent #
US 8,097,983 B2
Filed 05/08/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
INCREASING THE Q FACTOR OF A RESONATOR | ||
Patent #
US 20120001492A9
Filed 08/11/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Nigel Power LLC
|
Systems and methods for wireless power | ||
Patent #
US 8,115,448 B2
Filed 06/02/2008
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless non-radiative energy transfer | ||
Patent #
US 8,084,889 B2
Filed 03/31/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS ENERGY TRANSFER FOR IMPLANTABLE DEVICES | ||
Patent #
US 20120032522A1
Filed 06/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer for refrigerator application | ||
Patent #
US 8,106,539 B2
Filed 03/11/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
FLUSH-MOUNTED LOW-PROFILE RESONANT HOLE ANTENNA | ||
Patent #
US 20120038525A1
Filed 09/10/2009
|
Current Assignee
Advanced Automotive Antennas S.L.
|
Original Assignee
Advanced Automotive Antennas S.L.
|
Inductive repeater coil for an implantable device | ||
Patent #
US 8,131,378 B2
Filed 10/28/2007
|
Current Assignee
Second Sight Enterprises Incorporated
|
Original Assignee
Second Sight Enterprises Incorporated
|
LOW RESISTANCE ELECTRICAL CONDUCTOR | ||
Patent #
US 20120062345A1
Filed 08/31/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER, INCLUDING INTERFERENCE ENHANCEMENT | ||
Patent #
US 20120068549A1
Filed 11/03/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
WIRELESS TRANSMISSION OF SOLAR GENERATED POWER | ||
Patent #
US 20120086284A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MODULAR UPGRADES FOR WIRELESSLY POWERED TELEVISIONS | ||
Patent #
US 20120086867A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWERED TELEVISION | ||
Patent #
US 20120091795A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWERED PROJECTOR | ||
Patent #
US 20120091796A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWER TRANSFER WITHIN A CIRCUIT BREAKER | ||
Patent #
US 20120091820A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESSLY POWERED LAPTOP AND DESKTOP ENVIRONMENT | ||
Patent #
US 20120091794A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
ENERGIZED TABLETOP | ||
Patent #
US 20120091797A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
POSITION INSENSITIVE WIRELESS CHARGING | ||
Patent #
US 20120091950A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR ENERGIZING POWER TOOLS | ||
Patent #
US 20120091949A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
COMPUTER THAT WIRELESSLY POWERS ACCESSORIES | ||
Patent #
US 20120091819A1
Filed 10/06/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR PHOTOVOLTAIC PANELS | ||
Patent #
US 20120098350A1
Filed 10/19/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER WITH MULTI RESONATOR ARRAYS FOR VEHICLE APPLICATIONS | ||
Patent #
US 20120112534A1
Filed 10/17/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR VEHICLE APPLICATIONS | ||
Patent #
US 20120112538A1
Filed 11/03/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
SECURE WIRELESS ENERGY TRANSFER FOR VEHICLE APPLICATIONS | ||
Patent #
US 20120112531A1
Filed 11/03/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR VEHICLES | ||
Patent #
US 20120112535A1
Filed 10/19/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR VEHICLES | ||
Patent #
US 20120112536A1
Filed 10/19/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER FOR IN-VEHICLE APPLICATIONS | ||
Patent #
US 20120112532A1
Filed 11/03/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR VEHICLES | ||
Patent #
US 20120112691A1
Filed 10/18/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI-RESONATOR WIRELESS ENERGY TRANSFER INSIDE VEHICLES | ||
Patent #
US 20120119569A1
Filed 10/17/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR VEHICLES | ||
Patent #
US 20120119575A1
Filed 10/18/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
SAFETY SYSTEMS FOR WIRELESS ENERGY TRANSFER IN VEHICLE APPLICATIONS | ||
Patent #
US 20120119576A1
Filed 10/18/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR VEHICLES | ||
Patent #
US 20120119698A1
Filed 10/17/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Inductively chargeable audio devices | ||
Patent #
US 8,193,769 B2
Filed 01/25/2010
|
Current Assignee
Powermat Technologies Ltd.
|
Original Assignee
Powermat Technologies Ltd.
|
WIRELESS ENERGY TRANSFER FOR MEDICAL APPLICATIONS | ||
Patent #
US 20120139355A1
Filed 04/20/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER WITH HIGH-Q RESONATORS USING FIELD SHAPING TO IMPROVE K | ||
Patent #
US 20120153735A1
Filed 12/29/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER USING CONDUCTING SURFACES TO SHAPE FIELD AND IMPROVE K | ||
Patent #
US 20120153734A1
Filed 12/29/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER USING OBJECT POSITIONING FOR IMPROVED K | ||
Patent #
US 20120153736A1
Filed 12/29/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR COMPUTER PERIPHERAL APPLICATIONS | ||
Patent #
US 20120153732A1
Filed 11/05/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER SYSTEMS | ||
Patent #
US 20120153733A1
Filed 12/14/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER OVER DISTANCE USING FIELD SHAPING TO IMPROVE THE COUPLING FACTOR | ||
Patent #
US 20120153737A1
Filed 12/30/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER ACROSS VARIABLE DISTANCES USING FIELD SHAPING WITH MAGNETIC MATERIALS TO IMPROVE THE COUPLING FACTOR | ||
Patent #
US 20120153738A1
Filed 12/30/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR SUPPLYING POWER AND HEAT TO A DEVICE | ||
Patent #
US 20120153893A1
Filed 12/31/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
INTEGRATED REPEATERS FOR CELL PHONE APPLICATIONS | ||
Patent #
US 20120184338A1
Filed 03/23/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
SYSTEMS AND METHODS FOR WIRELESS POWER | ||
Patent #
US 20120206096A1
Filed 01/20/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Non-contact wireless communication apparatus, method of adjusting resonance frequency of non-contact wireless communication antenna, and mobile terminal apparatus | ||
Patent #
US 8,260,200 B2
Filed 11/14/2008
|
Current Assignee
Sony Corporation
|
Original Assignee
Sony Ericsson Mobile Communications AB
|
FLEXIBLE RESONATOR ATTACHMENT | ||
Patent #
US 20120223573A1
Filed 01/30/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER FOR APPLIANCES | ||
Patent #
US 20120228952A1
Filed 11/08/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER FOR FURNITURE APPLICATIONS | ||
Patent #
US 20120228953A1
Filed 11/08/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER FOR CLOTHING APPLICATIONS | ||
Patent #
US 20120228954A1
Filed 11/08/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY DISTRIBUTION SYSTEM | ||
Patent #
US 20120235500A1
Filed 09/14/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER USING REPEATER RESONATORS | ||
Patent #
US 20120235505A1
Filed 02/08/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER FOR OUTDOOR LIGHTING APPLICATIONS | ||
Patent #
US 20120235567A1
Filed 11/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER FOR LIGHTING APPLICATIONS | ||
Patent #
US 20120235566A1
Filed 11/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER WITH VARIABLE SIZE RESONATORS FOR IMPLANTED MEDICAL DEVICES | ||
Patent #
US 20120235633A1
Filed 10/21/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI-RESONATOR WIRELESS ENERGY TRANSFER FOR IMPLANTED MEDICAL DEVICES | ||
Patent #
US 20120235502A1
Filed 10/21/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI-RESONATOR WIRELESS ENERGY TRANSFER FOR MEDICAL APPLICATIONS | ||
Patent #
US 20120235501A1
Filed 10/21/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER FOR SENSORS | ||
Patent #
US 20120235504A1
Filed 11/08/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
SECURE WIRELESS ENERGY TRANSFER IN MEDICAL APPLICATIONS | ||
Patent #
US 20120235503A1
Filed 11/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER WITH VARIABLE SIZE RESONATORS FOR MEDICAL APPLICATIONS | ||
Patent #
US 20120235634A1
Filed 10/21/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER WITH RESONATOR ARRAYS FOR MEDICAL APPLICATIONS | ||
Patent #
US 20120239117A1
Filed 10/21/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI-RESONATOR WIRELESS ENERGY TRANSFER FOR APPLIANCES | ||
Patent #
US 20120242159A1
Filed 10/28/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI-RESONATOR WIRELESS ENERGY TRANSFER FOR EXTERIOR LIGHTING | ||
Patent #
US 20120242225A1
Filed 10/28/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS ENERGY TRANSFER FOR MEDICAL APPLICATIONS | ||
Patent #
US 20120256494A1
Filed 11/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer using field shaping to reduce loss | ||
Patent #
US 8,304,935 B2
Filed 12/28/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Low AC resistance conductor designs | ||
Patent #
US 20120280765A1
Filed 12/16/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer using magnetic materials to shape field and reduce loss | ||
Patent #
US 8,324,759 B2
Filed 12/28/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
RESONATOR OPTIMIZATIONS FOR WIRELESS ENERGY TRANSFER | ||
Patent #
US 20120313449A1
Filed 06/22/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Compact resonators for wireless energy transfer in vehicle applications | ||
Patent #
US 20120313742A1
Filed 06/28/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR PERSON WORN PERIPHERALS | ||
Patent #
US 20130007949A1
Filed 07/09/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWER COMPONENT SELECTION | ||
Patent #
US 20130020878A1
Filed 07/23/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
TUNABLE WIRELESS POWER ARCHITECTURES | ||
Patent #
US 20130033118A1
Filed 08/06/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWER COMPONENT SELECTION | ||
Patent #
US 20130038402A1
Filed 08/20/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
RESONATOR ENCLOSURE | ||
Patent #
US 20130057364A1
Filed 09/04/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
RECONFIGURABLE CONTROL ARCHITECTURES AND ALGORITHMS FOR ELECTRIC VEHICLE WIRELESS ENERGY TRANSFER SYSTEMS | ||
Patent #
US 20130062966A1
Filed 09/12/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS POWER TRANSMISSION APPARATUS | ||
Patent #
US 20120248884A1
Filed 05/06/2011
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
Wireless energy transfer for computer peripheral applications | ||
Patent #
US 8,400,017 B2
Filed 11/05/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer with high-Q capacitively loaded conducting loops | ||
Patent #
US 8,400,023 B2
Filed 12/23/2009
|
Current Assignee
Massachusetts Institute of Technology
|
Original Assignee
Massachusetts Institute of Technology
|
FOREIGN OBJECT DETECTION IN WIRELESS ENERGY TRANSFER SYSTEMS | ||
Patent #
US 20130069441A1
Filed 09/10/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
HIGH FREQUENCY PCB COILS | ||
Patent #
US 20130069753A1
Filed 09/17/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Low AC resistance conductor designs | ||
Patent #
US 8,410,636 B2
Filed 12/16/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR PACKAGING | ||
Patent #
US 20130099587A1
Filed 10/18/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI-RESONATOR WIRELESS ENERGY TRANSFER FOR SENSORS | ||
Patent #
US 20120248887A1
Filed 10/28/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI-RESONATOR WIRELESS ENERGY TRANSFER FOR LIGHTING | ||
Patent #
US 20120248981A1
Filed 10/28/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER WITH RESONATOR ARRAYS FOR MEDICAL APPLICATIONS | ||
Patent #
US 20120248888A1
Filed 11/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MULTI-RESONATOR WIRELESS ENERGY TRANSFER TO MOBILE DEVICES | ||
Patent #
US 20120248886A1
Filed 10/28/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Multi-resonator wireless energy transfer for exterior lighting | ||
Patent #
US 8,441,154 B2
Filed 10/28/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Magnetic induction signal repeater | ||
Patent #
US 8,457,547 B2
Filed 04/28/2009
|
Current Assignee
Cochlear Limited
|
Original Assignee
Cochlear Limited
|
Wireless energy transfer using conducting surfaces to shape field and improve K | ||
Patent #
US 8,461,722 B2
Filed 12/29/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer systems | ||
Patent #
US 8,461,719 B2
Filed 09/25/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer using conducting surfaces to shape fields and reduce loss | ||
Patent #
US 8,461,720 B2
Filed 12/28/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer using object positioning for low loss | ||
Patent #
US 8,461,721 B2
Filed 12/29/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Tunable wireless energy transfer for outdoor lighting applications | ||
Patent #
US 8,466,583 B2
Filed 11/07/2011
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER SYSTEMS | ||
Patent #
US 20130154389A1
Filed 02/21/2013
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER MODELING TOOL | ||
Patent #
US 20130159956A1
Filed 11/05/2012
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer over distance using field shaping to improve the coupling factor | ||
Patent #
US 8,471,410 B2
Filed 12/30/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer with high-Q resonators using field shaping to improve K | ||
Patent #
US 8,476,788 B2
Filed 12/29/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Increasing the Q factor of a resonator | ||
Patent #
US 8,482,157 B2
Filed 08/11/2008
|
Current Assignee
Qualcomm Inc.
|
Original Assignee
Qualcomm Inc.
|
Wireless energy transfer using variable size resonators and system monitoring | ||
Patent #
US 8,482,158 B2
Filed 12/28/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER SYSTEMS | ||
Patent #
US 20130175875A1
Filed 02/21/2013
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER FOR PROMOTIONAL ITEMS | ||
Patent #
US 20130175874A1
Filed 01/09/2013
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer resonator kit | ||
Patent #
US 8,487,480 B1
Filed 12/16/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer converters | ||
Patent #
US 8,497,601 B2
Filed 04/26/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
WIRELESS ENERGY TRANSFER RESONATOR KIT | ||
Patent #
US 20130200716A1
Filed 12/16/2009
|
Current Assignee
Witricity Corporation
|
Original Assignee
Qiang Li, David A. Schatz, Katherine Hall, Konrad J. Kulikowski, Marin Soljacic, Eric R. Giler, Morris P. Kesler, Andre B. Kurs, Andrew J. Campanella, Aristeidis Karalis, Ron Fiorello
|
WIRELESS ENERGY TRANSFER WITH REDUCED FIELDS | ||
Patent #
US 20130200721A1
Filed 01/28/2013
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
MECHANICALLY REMOVABLE WIRELESS POWER VEHICLE SEAT ASSEMBLY | ||
Patent #
US 20130221744A1
Filed 03/15/2013
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
Wireless energy transfer with feedback control for lighting applications | ||
Patent #
US 8,552,592 B2
Filed 02/02/2010
|
Current Assignee
Witricity Corporation
|
Original Assignee
Witricity Corporation
|
THERMOELECTRIC UNITS | ||
Patent #
US 3,780,425 A
Filed 01/25/1971
|
Current Assignee
United Kingdom Atomic Energy Authority
|
Original Assignee
United Kingdom Atomic Energy Authority
|
LARGE SODIUM VALVE ACTUATOR | ||
Patent #
US 3,871,176 A
Filed 03/08/1973
|
Current Assignee
Glen Elwin Schukei
|
Original Assignee
Combustion Engineering Incorporated
|
ENERGY TRANSLATING DEVICE | ||
Patent #
US 3,517,350 A
Filed 07/07/1969
|
Current Assignee
William D. Beaver
|
Original Assignee
William D. Beaver
|
MICROWAVE POWER RECEIVING ANTENNA | ||
Patent #
US 3,535,543 A
Filed 05/01/1969
|
Current Assignee
Carroll C. Dailey
|
Original Assignee
Carroll C. Dailey
|
26 Claims
-
1. A resonator for wireless power transfer comprising:
-
a conductor forming one or more loops and having an inductance L, a network of capacitors, having a capacitance, C, and a desired electrical parameter, coupled to the conductor, the network having at least one capacitor of a first type with a first temperature profile of the electrical parameter, and the network having at least one capacitor of a second type with a second temperature profile of the electrical parameter. - View Dependent Claims (2, 3, 4, 5, 6, 7, 8, 9)
-
-
10. A resonator for wireless power transfer comprising:
-
a conductor forming one or more loops, two or more types of electrical components having different temperature profiles for an electrical parameter, the electrical components forming a network connected to said conductor, wherein the electrical components are arranged such that the temperature profiles of the components are complementary and there is less change in the electrical parameter of a circuit comprising the network and the conductor due to a temperature change than when only a one type of component is used. - View Dependent Claims (11, 12, 13, 14, 15, 16, 17, 18, 19)
-
-
20. A resonator for wireless power transfer comprising:
-
a conductor forming one or more loops, at least one capacitor, having a temperature profile and connected to said conductor, wherein the at least one capacitor tunes a resonant frequency of the resonator and wherein the temperature profile of the at least one capacitor is chosen to detune the resonator from the resonant frequency when the temperature exceeds an operating range of the resonator. - View Dependent Claims (21, 22, 23, 24, 25, 26)
-
1 Specification
This application is a continuation-in-part of the following U.S. Applications: U.S. application Ser. No. 12/639,489 filed Dec. 16, 2009; and U.S. application Ser. No. 12/647,705 filed Dec. 28, 2009.
This application is a continuation-in-part of U.S. application Ser. No. 12/567,716 filed Sep. 25, 2009, which claims the benefit of the following U.S. Provisional App. No.: U.S. App. No. 61/100,721 filed Sep. 27, 2008; U.S. App. No. 61/108,743 filed Oct. 27, 2008; U.S. App. No. 61/147,386 filed Jan. 26, 2009; U.S. App. No. 61/152,086 filed Feb. 12, 2009; U.S. App. No. 61/178,508 filed May 15, 2009; U.S. App. No. 61/182,768 filed Jun. 1, 2009; U.S. App. No. 61/121,159 filed Dec. 9, 2008; U.S. App. No. 61/142,977 filed Jan. 7, 2009; U.S. App. No. 61/142,885 filed Jan. 6, 2009; U.S. App. No. 61/142,796 filed Jan. 6, 2009; U.S. App. No. 61/142,889 filed Jan. 6, 2009; U.S. App. No. 61/142,880 filed Jan. 6, 2009; U.S. App. No. 61/142,818 filed Jan. 6, 2009; U.S. App. No. 61/142,887 filed Jan. 6, 2009; U.S. App. No. 61/156,764 filed Mar. 2, 2009; U.S. App. No. 61/143,058 filed Jan. 7, 2009; U.S. App. No. 61/152,390 filed Feb. 13, 2009; U.S. App. No. 61/163,695 filed Mar. 26, 2009; U.S. App. No. 61/172,633 filed Apr. 24, 2009; U.S. App. No. 61/169,240 filed Apr. 14, 2009, U.S. App. No. 61/173,747 filed Apr. 29, 2009.
Each of the foregoing applications is incorporated herein by reference in its entirety.
1. Field
This disclosure relates to wireless energy transfer, also referred to as wireless power transmission.
2. Description of the Related Art
Energy or power may be transferred wirelessly using a variety of known radiative, or far-field, and non-radiative, or near-field, techniques. For example, radiative wireless information transfer using low-directionality antennas, such as those used in radio and cellular communications systems and home computer networks, may be considered wireless energy transfer. However, this type of radiative transfer is very inefficient because only a tiny portion of the supplied or radiated power, namely, that portion in the direction of, and overlapping with, the receiver is picked up. The vast majority of the power is radiated away in all the other directions and lost in free space. Such inefficient power transfer may be acceptable for data transmission, but is not practical for transferring useful amounts of electrical energy for the purpose of doing work, such as for powering or charging electrical devices. One way to improve the transfer efficiency of some radiative energy transfer schemes is to use directional antennas to confine and preferentially direct the radiated energy towards a receiver. However, these directed radiation schemes may require an uninterruptible line-of-sight and potentially complicated tracking and steering mechanisms in the case of mobile transmitters and/or receivers. In addition, such schemes may pose hazards to objects or people that cross or intersect the beam when modest to high amounts of power are being transmitted. A known non-radiative, or near-field, wireless energy transfer scheme, often referred to as either induction or traditional induction, does not (intentionally) radiate power, but uses an oscillating current passing through a primary coil, to generate an oscillating magnetic near-field that induces currents in a near-by receiving or secondary coil. Traditional induction schemes have demonstrated the transmission of modest to large amounts of power, however only over very short distances, and with very small offset tolerances between the primary power supply unit and the secondary receiver unit. Electric transformers and proximity chargers are examples of devices that utilize this known short range, near-field energy transfer scheme.
Therefore a need exists for a wireless power transfer scheme that is capable of transferring useful amounts of electrical power over mid-range distances or alignment offsets. Such a wireless power transfer scheme should enable useful energy transfer over greater distances and alignment offsets than those realized with traditional induction schemes, but without the limitations and risks inherent in radiative transmission schemes.
There is disclosed herein a non-radiative or near-field wireless energy transfer scheme that is capable of transmitting useful amounts of power over mid-range distances and alignment offsets. This inventive technique uses coupled electromagnetic resonators with long-lived oscillatory resonant modes to transfer power from a power supply to a power drain. The technique is general and may be applied to a wide range of resonators, even where the specific examples disclosed herein relate to electromagnetic resonators. If the resonators are designed such that the energy stored by the electric field is primarily confined within the structure and that the energy stored by the magnetic field is primarily in the region surrounding the resonator. Then, the energy exchange is mediated primarily by the resonant magnetic near-field. These types of resonators may be referred to as magnetic resonators. If the resonators are designed such that the energy stored by the magnetic field is primarily confined within the structure and that the energy stored by the electric field is primarily in the region surrounding the resonator. Then, the energy exchange is mediated primarily by the resonant electric near-field. These types of resonators may be referred to as electric resonators. Either type of resonator may also be referred to as an electromagnetic resonator. Both types of resonators are disclosed herein.
The omni-directional but stationary (non-lossy) nature of the near-fields of the resonators we disclose enables efficient wireless energy transfer over mid-range distances, over a wide range of directions and resonator orientations, suitable for charging, powering, or simultaneously powering and charging a variety of electronic devices. As a result, a system may have a wide variety of possible applications where a first resonator, connected to a power source, is in one location, and a second resonator, potentially connected to electrical/electronic devices, batteries, powering or charging circuits, and the like, is at a second location, and where the distance from the first resonator to the second resonator is on the order of centimeters to meters. For example, a first resonator connected to the wired electricity grid could be placed on the ceiling of a room, while other resonators connected to devices, such as robots, vehicles, computers, communication devices, medical devices, and the like, move about within the room, and where these devices are constantly or intermittently receiving power wirelessly from the source resonator. From this one example, one can imagine many applications where the systems and methods disclosed herein could provide wireless power across mid-range distances, including consumer electronics, industrial applications, infrastructure power and lighting, transportation vehicles, electronic games, military applications, and the like.
Energy exchange between two electromagnetic resonators can be optimized when the resonators are tuned to substantially the same frequency and when the losses in the system are minimal. Wireless energy transfer systems may be designed so that the “coupling-time” between resonators is much shorter than the resonators'"'"' “loss-times”. Therefore, the systems and methods described herein may utilize high quality factor (high-Q) resonators with low intrinsic-loss rates. In addition, the systems and methods described herein may use sub-wavelength resonators with near-fields that extend significantly longer than the characteristic sizes of the resonators, so that the near-fields of the resonators that exchange energy overlap at mid-range distances. This is a regime of operation that has not been practiced before and that differs significantly from traditional induction designs.
It is important to appreciate the difference between the high-Q magnetic resonator scheme disclosed here and the known close-range or proximity inductive schemes, namely, that those known schemes do not conventionally utilize high-Q resonators. Using coupled-mode theory (CMT), (see, for example, Waves and Fields in Optoelectronics, H. A. Haus, Prentice Hall, 1984), one may show that a high-Q resonator-coupling mechanism can enable orders of magnitude more efficient power delivery between resonators spaced by mid-range distances than is enabled by traditional inductive schemes. Coupled high-Q resonators have demonstrated efficient energy transfer over mid-range distances and improved efficiencies and offset tolerances in short range energy transfer applications.
The systems and methods described herein may provide for near-field wireless energy transfer via strongly coupled high-Q resonators, a technique with the potential to transfer power levels from picowatts to kilowatts, safely, and over distances much larger than have been achieved using traditional induction techniques. Efficient energy transfer may be realized for a variety of general systems of strongly coupled resonators, such as systems of strongly coupled acoustic resonators, nuclear resonators, mechanical resonators, and the like, as originally described by researchers at M.I.T. in their publications, “Efficient wireless non-radiative mid-range energy transfer”, Annals of Physics, vol. 323, Issue 1, p. 34 (2008) and “Wireless Power Transfer via Strongly Coupled Magnetic Resonances”, Science, vol. 317, no. 5834, p. 83, (2007). Disclosed herein are electromagnetic resonators and systems of coupled electromagnetic resonators, also referred to more specifically as coupled magnetic resonators and coupled electric resonators, with operating frequencies below 10 GHz.
This disclosure describes wireless energy transfer technologies, also referred to as wireless power transmission technologies. Throughout this disclosure, we may use the terms wireless energy transfer, wireless power transfer, wireless power transmission, and the like, interchangeably. We may refer to supplying energy or power from a source, an AC or DC source, a battery, a source resonator, a power supply, a generator, a solar panel, and thermal collector, and the like, to a device, a remote device, to multiple remote devices, to a device resonator or resonators, and the like. We may describe intermediate resonators that extend the range of the wireless energy transfer system by allowing energy to hop, transfer through, be temporarily stored, be partially dissipated, or for the transfer to be mediated in any way, from a source resonator to any combination of other device and intermediate resonators, so that energy transfer networks, or strings, or extended paths may be realized. Device resonators may receive energy from a source resonator, convert a portion of that energy to electric power for powering or charging a device, and simultaneously pass a portion of the received energy onto other device or mobile device resonators. Energy may be transferred from a source resonator to multiple device resonators, significantly extending the distance over which energy may be wirelessly transferred. The wireless power transmission systems may be implemented using a variety of system architectures and resonator designs. The systems may include a single source or multiple sources transmitting power to a single device or multiple devices. The resonators may be designed to be source or device resonators, or they may be designed to be repeaters. In some cases, a resonator may be a device and source resonator simultaneously, or it may be switched from operating as a source to operating as a device or a repeater. One skilled in the art will understand that a variety of system architectures may be supported by the wide range of resonator designs and functionalities described in this application.
In the wireless energy transfer systems we describe, remote devices may be powered directly, using the wirelessly supplied power or energy, or the devices may be coupled to an energy storage unit such as a battery, a super-capacitor, an ultra-capacitor, or the like (or other kind of power drain), where the energy storage unit may be charged or re-charged wirelessly, and/or where the wireless power transfer mechanism is simply supplementary to the main power source of the device. The devices may be powered by hybrid battery/energy storage devices such as batteries with integrated storage capacitors and the like. Furthermore, novel battery and energy storage devices may be designed to take advantage of the operational improvements enabled by wireless power transmission systems.
Other power management scenarios include using wirelessly supplied power to recharge batteries or charge energy storage units while the devices they power are turned off, in an idle state, in a sleep mode, and the like. Batteries or energy storage units may be charged or recharged at high (fast) or low (slow) rates. Batteries or energy storage units may be trickle charged or float charged. Multiple devices may be charged or powered simultaneously in parallel or power delivery to multiple devices may be serialized such that one or more devices receive power for a period of time after which other power delivery is switched to other devices. Multiple devices may share power from one or more sources with one or more other devices either simultaneously, or in a time multiplexed manner, or in a frequency multiplexed manner, or in a spatially multiplexed manner, or in an orientation multiplexed manner, or in any combination of time and frequency and spatial and orientation multiplexing. Multiple devices may share power with each other, with at least one device being reconfigured continuously, intermittently, periodically, occasionally, or temporarily, to operate as wireless power sources. It would be understood by one of ordinary skill in the art that there are a variety of ways to power and/or charge devices, and the variety of ways could be applied to the technologies and applications described herein.
Wireless energy transfer has a variety of possible applications including for example, placing a source (e.g. one connected to the wired electricity grid) on the ceiling, under the floor, or in the walls of a room, while devices such as robots, vehicles, computers, PDAs or similar are placed or move freely within the room. Other applications may include powering or recharging electric-engine vehicles, such as buses and/or hybrid cars and medical devices, such as wearable or implantable devices. Additional example applications include the ability to power or recharge autonomous electronics (e.g. laptops, cell-phones, portable music players, house-hold robots, GPS navigation systems, displays, etc), sensors, industrial and manufacturing equipment, medical devices and monitors, home appliances and tools (e.g. lights, fans, drills, saws, heaters, displays, televisions, counter-top appliances, etc.), military devices, heated or illuminated clothing, communications and navigation equipment, including equipment built into vehicles, clothing and protective-wear such as helmets, body armor and vests, and the like, and the ability to transmit power to physically isolated devices such as to implanted medical devices, to hidden, buried, implanted or embedded sensors or tags, to and/or from roof-top solar panels to indoor distribution panels, and the like.
In one aspect, disclosed herein is a system including a source resonator having a Q-factor Q1 and a characteristic size x1, coupled to a power generator with direct electrical connections; and a second resonator having a Q-factor Q2 and a characteristic size x2, coupled to a load with direct electrical connections, and located a distance D from the source resonator, wherein the source resonator and the second resonator are coupled to exchange energy wirelessly among the source resonator and the second resonator in order to transmit power from the power generator to the load, and wherein √{square root over (Q1Q2)} is greater than 100.
Q1 may be greater than 100 and Q2 may be less than 100. Q1 may be greater than 100 and Q2 may be greater than 100. A useful energy exchange may be maintained over an operating distance from 0 to D, where D is larger than the smaller of x1 and x2. At least one of the source resonator and the second resonator may be a coil of at least one turn of a conducting material connected to a first network of capacitors. The first network of capacitors may include at least one tunable capacitor. The direct electrical connections of at least one of the source resonator to the ground terminal of the power generator and the second resonator to the ground terminal of the load may be made at a point on an axis of electrical symmetry of the first network of capacitors. The first network of capacitors may include at least one tunable butterfly-type capacitor, wherein the direct electrical connection to the ground terminal is made on a center terminal of the at least one tunable butterfly-type capacitor. The direct electrical connection of at least one of the source resonator to the power generator and the second resonator to the load may be made via a second network of capacitors, wherein the first network of capacitors and the second network of capacitors form an impedance matching network. The impedance matching network may be designed to match the coil to a characteristic impedance of the power generator or the load at a driving frequency of the power generator.
At least one of the first network of capacitors and the second network of capacitors may include at least one tunable capacitor. The first network of capacitors and the second network of capacitors may be adjustable to change an impedance of the impedance matching network at a driving frequency of the power generator. The first network of capacitors and the second network of capacitors may be adjustable to match the coil to the characteristic impedance of the power generator or the load at a driving frequency of the power generator. At least one of the first network of capacitors and the second network of capacitors may include at least one fixed capacitor that reduces a voltage across the at least one tunable capacitor. The direct electrical connections of at least one of the source resonator to the power generator and the second resonator to the load may be configured to substantially preserve a resonant mode. At least one of the source resonator and the second resonator may be a tunable resonator. The source resonator may be physically separated from the power generator and the second resonator may be physically separated from the load. The second resonator may be coupled to a power conversion circuit to deliver DC power to the load. The second resonator may be coupled to a power conversion circuit to deliver AC power to the load. The second resonator may be coupled to a power conversion circuit to deliver both AC and DC power to the load. The second resonator may be coupled to a power conversion circuit to deliver power to a plurality of loads.
In another aspect, a system disclosed herein includes a source resonator having a Q-factor Q1 and a characteristic size x1, and a second resonator having a Q-factor Q2 and a characteristic size x2, and located a distance D from the source resonator; wherein the source resonator and the second resonator are coupled to exchange energy wirelessly among the source resonator and the second resonator; and wherein √{square root over (Q1Q2)} is greater than 100, and wherein at least one of the resonators is enclosed in a low loss tangent material.
In another aspect, a system disclosed herein includes a source resonator having a Q-factor Q1 and a characteristic size x1, and a second resonator having a Q-factor Q2 and a characteristic size x2, and located a distance D from the source resonator; wherein the source resonator and the second resonator are coupled to exchange energy wirelessly among the source resonator and the second resonator, and wherein √{square root over (Q1Q2)} is greater than 100; and wherein at least one of the resonators includes a coil of a plurality of turns of a conducting material connected to a network of capacitors, wherein the plurality of turns are in a common plane, and wherein a characteristic thickness of the at least one of the resonators is much less than a characteristic size of the at least one of the resonators.
Throughout this disclosure we may refer to the certain circuit components such as capacitors, inductors, resistors, diodes, switches and the like as circuit components or elements. We may also refer to series and parallel combinations of these components as elements, networks, topologies, circuits, and the like. We may describe combinations of capacitors, diodes, varactors, transistors, and/or switches as adjustable impedance networks, tuning networks, matching networks, adjusting elements, and the like. We may also refer to “self-resonant” objects that have both capacitance, and inductance distributed (or partially distributed, as opposed to solely lumped) throughout the entire object. It would be understood by one of ordinary skill in the art that adjusting and controlling variable components within a circuit or network may adjust the performance of that circuit or network and that those adjustments may be described generally as tuning, adjusting, matching, correcting, and the like. Other methods to tune or adjust the operating point of the wireless power transfer system may be used alone, or in addition to adjusting tunable components such as inductors and capacitors, or banks of inductors and capacitors.
Unless otherwise defined, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this disclosure belongs. In case of conflict with publications, patent applications, patents, and other references mentioned or incorporated herein by reference, the present specification, including definitions, will control.
Any of the features described above may be used, alone or in combination, without departing from the scope of this disclosure. Other features, objects, and advantages of the systems and methods disclosed herein will be apparent from the following detailed description and figures.
As described above, this disclosure relates to coupled electromagnetic resonators with long-lived oscillatory resonant modes that may wirelessly transfer power from a power supply to a power drain. However, the technique is not restricted to electromagnetic resonators, but is general and may be applied to a wide variety of resonators and resonant objects. Therefore, we first describe the general technique, and then disclose electromagnetic examples for wireless energy transfer.
Resonators
A resonator may be defined as a system that can store energy in at least two different forms, and where the stored energy is oscillating between the two forms. The resonance has a specific oscillation mode with a resonant (modal) frequency, f, and a resonant (modal) field. The angular resonant frequency, ω, may be defined as ω=2πf, the resonant wavelength, λ, may be defined as λ=c/f, where c is the speed of light, and the resonant period, T, may be defined as T=1/f=2π/ω. In the absence of loss mechanisms, coupling mechanisms or external energy supplying or draining mechanisms, the total resonator stored energy, W, would stay fixed and the two forms of energy would oscillate, wherein one would be maximum when the other is minimum and vice versa.
In the absence of extraneous materials or objects, the energy in the resonator 102 shown in
where the variable a(t) is the resonant field amplitude, defined so that the energy contained within the resonator is given by |a(t)|2. Γ is the intrinsic energy decay or loss rate (e.g. due to absorption and radiation losses).
The Quality Factor, or Q-factor, or Q, of the resonator, which characterizes the energy decay, is inversely proportional to these energy losses. It may be defined as Q=ω*W/P, where P is the time-averaged power lost at steady state. That is, a resonator 102 with a high-Q has relatively low intrinsic losses and can store energy for a relatively long time. Since the resonator loses energy at its intrinsic decay rate, 2Γ, its Q, also referred to as its intrinsic Q, is given by Q=ω/2Γ. The quality factor also represents the number of oscillation periods, T, it takes for the energy in the resonator to decay by a factor of e.
As described above, we define the quality factor or Q of the resonator as that due only to intrinsic loss mechanisms. A subscript index such as Q1, indicates the resonator (resonator 1 in this case) to which the Q refers.
Extraneous objects and/or additional resonators in the vicinity of a first resonator may perturb or load the first resonator, thereby perturbing or loading the Q of the first resonator, depending on a variety of factors such as the distance between the resonator and object or other resonator, the material composition of the object or other resonator, the structure of the first resonator, the power in the first resonator, and the like. Unintended external energy losses or coupling mechanisms to extraneous materials and objects in the vicinity of the resonators may be referred to as “perturbing” the Q of a resonator, and may be indicated by a subscript within rounded parentheses, ( ). Intended external energy losses, associated with energy transfer via coupling to other resonators and to generators and loads in the wireless energy transfer system may be referred to as “loading” the Q of the resonator, and may be indicated by a subscript within square brackets, [ ].
The Q of a resonator 102 connected or coupled to a power generator, g, or load 302, l, may be called the “loaded quality factor” or the “loaded Q” and may be denoted by Q[g] or Q[l], as illustrated in
In some of the discussion herein, we define the “loading quality factor” or the “loading Q” due to a power generator or load connected to the resonator, as δQ[l], where, 1/δQ[l]≡1/Q[l]−1/Q . Note that the larger the loading Q, δQ[l], of a generator or load, the less the loaded Q, Q[l], deviates from the unloaded Q of the resonator.
The Q of a resonator in the presence of an extraneous object 402, p, that is not intended to be part of the energy transfer system may be called the “perturbed quality factor” or the “perturbed Q” and may be denoted by Q(p), as illustrated in
In some of the discussion herein, we define the “perturbing quality factor” or the “perturbing Q” due to an extraneous object, p, as δQ(p), where 1/δQ(p)≡1/Q(p)−1/Q. As stated before, the perturbing quality factor may be due to multiple extraneous objects, p1, p2, etc. or a set of extraneous objects, {p}. The larger the perturbing Q, δQ(p), of an object, the less the perturbed Q, Q(p), deviates from the unperturbed Q of the resonator.
In some of the discussion herein, we also define Θ(p)≡Q(p)/Q and call it the “quality factor insensitivity” or the “Q-insensitivity” of the resonator in the presence of an extraneous object. A subscript index, such as Θ1(p), indicates the resonator to which the perturbed and unperturbed quality factors are referring, namely, Θ1(p)≡Q1(p)/Q1.
Note that the quality factor, Q, may also be characterized as “unperturbed”, when necessary to distinguish it from the perturbed quality factor, Q(p), and “unloaded”, when necessary to distinguish it from the loaded quality factor, Q[l]. Similarly, the perturbed quality factor, Q(p), may also be characterized as “unloaded”, when necessary to distinguish them from the loaded perturbed quality factor, Q(p)[l].
Coupled Resonators
Resonators having substantially the same resonant frequency, coupled through any portion of their near-fields may interact and exchange energy. There are a variety of physical pictures and models that may be employed to understand, design, optimize and characterize this energy exchange. One way to describe and model the energy exchange between two coupled resonators is using coupled mode theory (CMT).
In coupled mode theory, the resonator fields obey the following set of linear equations:
where the indices denote different resonators and κmn are the coupling coefficients between the resonators. For a reciprocal system, the coupling coefficients may obey the relation κmn=κnm. Note that, for the purposes of the present specification, far-field radiation interference effects will be ignored and thus the coupling coefficients will be considered real. Furthermore, since in all subsequent calculations of system performance in this specification the coupling coefficients appear only with their square, κmn2, we use κmn to denote the absolute value of the real coupling coefficients.
Note that the coupling coefficient, κmn, from the CMT described above is related to the so-called coupling factor, kmn, between resonators m and n by kmn=2κmn/√{square root over (ωmωn)}. We define a “strong-coupling factor”, Umn, as the ratio of the coupling and loss rates between resonators m and n, by Umn=κmn/√{square root over (ΓmΓn)}=kmn√{square root over (QmQn)}.
The quality factor of a resonator m, in the presence of a similar frequency resonator n or additional resonators, may be loaded by that resonator n or additional resonators, in a fashion similar to the resonator being loaded by a connected power generating or consuming device. The fact that resonator m may be loaded by resonator n and vice versa is simply a different way to see that the resonators are coupled.
The loaded Q'"'"'s of the resonators in these cases may be denoted as Qm[n] and Qn[m]. For multiple resonators or loading supplies or devices, the total loading of a resonator may be determined by modeling each load as a resistive loss, and adding the multiple loads in the appropriate parallel and/or series combination to determine the equivalent load of the ensemble.
In some of the discussion herein, we define the “loading quality factor” or the “loading Qm” of resonator m due to resonator n as δQm[n], where 1/δQm[n]≡1/Qm[n]−1/Qm. Note that resonator n is also loaded by resonator m and its “loading Qn” is given by 1/δQn[m]≡1/Qn[m]−1/Qn.
When one or more of the resonators are connected to power generators or loads, the set of linear equations is modified to:
where s+m(t) and s−m(t) are respectively the amplitudes of the fields coming from a generator into the resonator m and going out of the resonator m either back towards the generator or into a load, defined so that the power they carry is given by |s+m(t)|2 and |s−m(t)|2. The loading coefficients κm relate to the rate at which energy is exchanged between the resonator m and the generator or load connected to it.
Note that the loading coefficient, κm, from the CMT described above is related to the loading quality factor, δQm[l], defined earlier, by δQm[l]=ωm/2κm.
We define a “strong-loading factor”, Um[l], as the ratio of the loading and loss rates of resonator m, Um[l]=κm/Γm=Qm/δQm[l].
The power generator may be constantly driving the source resonator at a constant driving frequency, f, corresponding to an angular driving frequency, ω, where ω=2πf.
In this case, the efficiency, η=|s−d|2/|s+s|2, of the power transmission from the generator to the load (via the source and device resonators) is maximized under the following conditions: The source resonant frequency, the device resonant frequency and the generator driving frequency have to be matched, namely
ωs=ωd=ω.
Furthermore, the loading Q of the source resonator due to the generator, δQs[g], has to be matched (equal) to the loaded Q of the source resonator due to the device resonator and the load, Qs[dl], and inversely the loading Q of the device resonator due to the load, δQd[l], has to be matched (equal) to the loaded Q of the device resonator due to the source resonator and the generator, Qd[sg], namely
δQs[g]=Qs[dl] and δQd[l]=Qd[sg].
These equations determine the optimal loading rates of the source resonator by the generator and of the device resonator by the load as
Ud[l]=κd/Γd=Qd/δQd[l]=√{square root over (1+U2)}=√{square root over (1+(κ/√{square root over (ΓsΓd)})2)}=Qs/δQs[g]=κs/Γs=Us[g].
Note that the above frequency matching and Q matching conditions are together known as “impedance matching” in electrical engineering.
Under the above conditions, the maximized efficiency is a monotonically increasing function of only the strong-coupling factor, U=κ/√{square root over (ΓsΓd)}=k√{square root over (QsQd)}, between the source and device resonators and is given by, η=U2/(1+√{square root over (1+U2)})2, as shown in
Since a large U=κ/√{square root over (ΓsΓd)}=(2κ/√{square root over (ωsωd)})√{square root over (QsQd)} is desired in certain circumstances, resonators may be used that are high-Q. The Q of each resonator may be high. The geometric mean of the resonator Q'"'"'s, √{square root over (QsQd)} may also or instead be high.
The coupling factor, k, is a number between 0≦k≦1, and it may be independent (or nearly independent) of the resonant frequencies of the source and device resonators, rather it may determined mostly by their relative geometry and the physical decay-law of the field mediating their coupling. In contrast, the coupling coefficient, κ=k√{square root over (ωsωd)}/2, may be a strong function of the resonant frequencies. The resonant frequencies of the resonators may be chosen preferably to achieve a high Q rather than to achieve a low Γ, as these two goals may be achievable at two separate resonant frequency regimes.
A high-Q resonator may be defined as one with Q>100. Two coupled resonators may be referred to as a system of high-Q resonators when each resonator has a Q greater than 100, Qs>100 and Qd>100. In other implementations, two coupled resonators may be referred to as a system of high-Q resonators when the geometric mean of the resonator Q'"'"'s is greater than 100, √{square root over (QsQd)}>100.
The resonators may be named or numbered. They may be referred to as source resonators, device resonators, first resonators, second resonators, repeater resonators, and the like. It is to be understood that while two resonators are shown in
The analysis of a single source and a single device resonator may be extended to multiple source resonators and/or multiple device resonators and/or multiple intermediate resonators. In such an analysis, the conclusion may be that large strong-coupling factors, Umn, between at least some or all of the multiple resonators is preferred for a high system efficiency in the wireless energy transfer. Again, implementations may use source, device and intermediate resonators that have a high Q. The Q of each resonator may be high. The geometric mean √{square root over (QmQn)} of the Q'"'"'s for pairs of resonators m and n, for which a large Umn is desired, may also or instead be high.
Note that since the strong-coupling factor of two resonators may be determined by the relative magnitudes of the loss mechanisms of each resonator and the coupling mechanism between the two resonators, the strength of any or all of these mechanisms may be perturbed in the presence of extraneous objects in the vicinity of the resonators as described above.
Continuing the conventions for labeling from the previous sections, we describe k as the coupling factor in the absence of extraneous objects or materials. We denote the coupling factor in the presence of an extraneous object, p, as k(p), and call it the “perturbed coupling factor” or the “perturbed k”. Note that the coupling factor, k, may also be characterized as “unperturbed”, when necessary to distinguish from the perturbed coupling factor k(p).
We define δk(p)≡k(p)−k and we call it the “perturbation on the coupling factor” or the “perturbation on k” due to an extraneous object, p.
We also define β(p)≡k(p)/k and we call it the “coupling factor insensitivity” or the “k-insensitivity”. Lower indices, such as β12(p), indicate the resonators to which the perturbed and unperturbed coupling factor is referred to, namely β12(p)≡k12(p)/k12.
Similarly, we describe U as the strong-coupling factor in the absence of extraneous objects. We denote the strong-coupling factor in the presence of an extraneous object, p, as U(p), U(p)=k(p)√{square root over (Q1(p)Q2(p))}{square root over (Q1(p)Q2(p))}, and call it the “perturbed strong-coupling factor” or the “perturbed U”. Note that the strong-coupling factor U may also be characterized as “unperturbed”, when necessary to distinguish from the perturbed strong-coupling factor U(p). Note that the strong-coupling factor U may also be characterized as “unperturbed”, when necessary to distinguish from the perturbed strong-coupling factor U(p).
We define δU(p)≡U(p)−U and call it the “perturbation on the strong-coupling factor” or the “perturbation on U” due to an extraneous object, p.
We also define Ξ(p)=U(p)/U and call it the “strong-coupling factor insensitivity” or the “U-insensitivity”. Lower indices, such as Ξ12(p), indicate the resonators to which the perturbed and unperturbed coupling factor refers, namely Ξ12(p)≡U12(p)/U12.
The efficiency of the energy exchange in a perturbed system may be given by the same formula giving the efficiency of the unperturbed system, where all parameters such as strong-coupling factors, coupling factors, and quality factors are replaced by their perturbed equivalents. For example, in a system of wireless energy transfer including one source and one device resonator, the optimal efficiency may calculated as η(p)=[U(p)/(1+√{square root over (1+U(p)2)})]2. Therefore, in a system of wireless energy exchange which is perturbed by extraneous objects, large perturbed strong-coupling factors, Umn(p), between at least some or all of the multiple resonators may be desired for a high system efficiency in the wireless energy transfer. Source, device and/or intermediate resonators may have a high Q(p).
Some extraneous perturbations may sometimes be detrimental for the perturbed strong-coupling factors (via large perturbations on the coupling factors or the quality factors). Therefore, techniques may be used to reduce the effect of extraneous perturbations on the system and preserve large strong-coupling factor insensitivites.
Efficiency of Energy Exchange
The so-called “useful” energy in a useful energy exchange is the energy or power that must be delivered to a device (or devices) in order to power or charge the device. The transfer efficiency that corresponds to a useful energy exchange may be system or application dependent. For example, high power vehicle charging applications that transfer kilowatts of power may need to be at least 80% efficient in order to supply useful amounts of power resulting in a useful energy exchange sufficient to recharge a vehicle battery, without significantly heating up various components of the transfer system. In some consumer electronics applications, a useful energy exchange may include any energy transfer efficiencies greater than 10%, or any other amount acceptable to keep rechargeable batteries “topped off” and running for long periods of time. For some wireless sensor applications, transfer efficiencies that are much less than 1% may be adequate for powering multiple low power sensors from a single source located a significant distance from the sensors. For still other applications, where wired power transfer is either impossible or impractical, a wide range of transfer efficiencies may be acceptable for a useful energy exchange and may be said to supply useful power to devices in those applications. In general, an operating distance is any distance over which a useful energy exchange is or can be maintained according to the principles disclosed herein.
A useful energy exchange for a wireless energy transfer in a powering or recharging application may be efficient, highly efficient, or efficient enough, as long as the wasted energy levels, heat dissipation, and associated field strengths are within tolerable limits. The tolerable limits may depend on the application, the environment and the system location. Wireless energy transfer for powering or recharging applications may be efficient, highly efficient, or efficient enough, as long as the desired system performance may be attained for the reasonable cost restrictions, weight restrictions, size restrictions, and the like. Efficient energy transfer may be determined relative to that which could be achieved using traditional inductive techniques that are not high-Q systems. Then, the energy transfer may be defined as being efficient, highly efficient, or efficient enough, if more energy is delivered than could be delivered by similarly sized coil structures in traditional inductive schemes over similar distances or alignment offsets.
Note that, even though certain frequency and Q matching conditions may optimize the system efficiency of energy transfer, these conditions may not need to be exactly met in order to have efficient enough energy transfer for a useful energy exchange. Efficient energy exchange may be realized so long as the relative offset of the resonant frequencies (|ωm−ωn|/√{square root over (ωmωn)}) is less than approximately the maximum among 1/Qm(p), 1/Qn(p) and kmn(p). The Q matching condition may be less critical than the frequency matching condition for efficient energy exchange. The degree by which the strong-loading factors, Um[l], of the resonators due to generators and/or loads may be away from their optimal values and still have efficient enough energy exchange depends on the particular system, whether all or some of the generators and/or loads are Q-mismatched and so on.
Therefore, the resonant frequencies of the resonators may not be exactly matched, but may be matched within the above tolerances. The strong-loading factors of at least some of the resonators due to generators and/or loads may not be exactly matched to their optimal value. The voltage levels, current levels, impedance values, material parameters, and the like may not be at the exact values described in the disclosure but will be within some acceptable tolerance of those values. The system optimization may include cost, size, weight, complexity, and the like, considerations, in addition to efficiency, Q, frequency, strong coupling factor, and the like, considerations. Some system performance parameters, specifications, and designs may be far from optimal in order to optimize other system performance parameters, specifications and designs.
In some applications, at least some of the system parameters may be varying in time, for example because components, such as sources or devices, may be mobile or aging or because the loads may be variable or because the perturbations or the environmental conditions are changing etc. In these cases, in order to achieve acceptable matching conditions, at least some of the system parameters may need to be dynamically adjustable or tunable. All the system parameters may be dynamically adjustable or tunable to achieve approximately the optimal operating conditions. However, based on the discussion above, efficient enough energy exchange may be realized even if some system parameters are not variable. In some examples, at least some of the devices may not be dynamically adjusted. In some examples, at least some of the sources may not be dynamically adjusted. In some examples, at least some of the intermediate resonators may not be dynamically adjusted. In some examples, none of the system parameters may be dynamically adjusted.
Electromagnetic Resonators
The resonators used to exchange energy may be electromagnetic resonators. In such resonators, the intrinsic energy decay rates, Γm, are given by the absorption (or resistive) losses and the radiation losses of the resonator.
The resonator may be constructed such that the energy stored by the electric field is primarily confined within the structure and that the energy stored by the magnetic field is primarily in the region surrounding the resonator. Then, the energy exchange is mediated primarily by the resonant magnetic near-field. These types of resonators may be referred to as magnetic resonators.
The resonator may be constructed such that the energy stored by the magnetic field is primarily confined within the structure and that the energy stored by the electric field is primarily in the region surrounding the resonator. Then, the energy exchange is mediated primarily by the resonant electric near-field. These types of resonators may be referred to as electric resonators.
Note that the total electric and magnetic energies stored by the resonator have to be equal, but their localizations may be quite different. In some cases, the ratio of the average electric field energy to the average magnetic field energy specified at a distance from a resonator may be used to characterize or describe the resonator.
Electromagnetic resonators may include an inductive element, a distributed inductance, or a combination of inductances with inductance, L, and a capacitive element, a distributed capacitance, or a combination of capacitances, with capacitance, C. A minimal circuit model of an electromagnetic resonator 102 is shown in
The resonators 102 shown in
The inductor 108 and capacitor 104 of an electromagnetic resonator 102 may be bulk circuit elements, or the inductance and capacitance may be distributed and may result from the way the conductors are formed, shaped, or positioned, in the structure. For example, the inductor 108 may be realized by shaping a conductor to enclose a surface area, as shown in
where μ0 is the magnetic permeability of free space, x, is the radius of the enclosed circular surface area and, a, is the radius of the conductor used to form the inductor loop. A more precise value of the inductance of the loop may be calculated analytically or numerically.
The inductance for other cross-section conductors, arranged to form other enclosed surface shapes, areas, sizes, and the like, and of any number of wire turns, may be calculated analytically, numerically or it may be determined by measurement. The inductance may be realized using inductor elements, distributed inductance, networks, arrays, series and parallel combinations of inductors and inductances, and the like. The inductance may be fixed or variable and may be used to vary impedance matching as well as resonant frequency operating conditions.
There are a variety of ways to realize the capacitance required to achieve the desired resonant frequency for a resonator structure. Capacitor plates 110 may be formed and utilized as shown in
It is to be understood that the inductance and capacitance in an electromagnetic resonator 102 may be lumped, distributed, or a combination of lumped and distributed inductance and capacitance and that electromagnetic resonators may be realized by combinations of the various elements, techniques and effects described herein.
Electromagnetic resonators 102 may be include inductors, inductances, capacitors, capacitances, as well as additional circuit elements such as resistors, diodes, switches, amplifiers, diodes, transistors, transformers, conductors, connectors and the like.
Resonant Frequency of an Electromagnetic Resonator
An electromagnetic resonator 102 may have a characteristic, natural, or resonant frequency determined by its physical properties. This resonant frequency is the frequency at which the energy stored by the resonator oscillates between that stored by the electric field, WE, (WE=q2/2C, where q is the charge on the capacitor, C) and that stored by the magnetic field, WB, (WB=Li2/2, where i is the current through the inductor, L) of the resonator. In the absence of any losses in the system, energy would continually be exchanged between the electric field in the capacitor 104 and the magnetic field in the inductor 108. The frequency at which this energy is exchanged may be called the characteristic frequency, the natural frequency, or the resonant frequency of the resonator, and is given by ω,
The resonant frequency of the resonator may be changed by tuning the inductance, L, and/or the capacitance, C, of the resonator. The resonator frequency may be design to operate at the so-called ISM (Industrial, Scientific and Medical) frequencies as specified by the FCC. The resonator frequency may be chosen to meet certain field limit specifications, specific absorption rate (SAR) limit specifications, electromagnetic compatibility (EMC) specifications, electromagnetic interference (EMI) specifications, component size, cost or performance specifications, and the like.
Quality Factor of an Electromagnetic Resonator
The energy in the resonators 102 shown in
where ω, is the resonant frequency, L, is the total inductance of the resonator and the resistance for the conductor used to form the inductor, for example, may be given by Rabs=lρ/A, (l is the length of the wire, ρ is the resistivity of the conductor material, and A is the cross-sectional area over which current flows in the wire). For alternating currents, the cross-sectional area over which current flows may be less than the physical cross-sectional area of the conductor owing to the skin effect. Therefore, high-Q magnetic resonators may be composed of conductors with high conductivity, relatively large surface areas and/or with specially designed profiles (e.g. Litz wire) to minimize proximity effects and reduce the AC resistance.
The magnetic resonator structures may include high-Q inductive elements composed of high conductivity wire, coated wire, Litz wire, ribbon, strapping or plates, tubing, paint, gels, traces, and the like. The magnetic resonators may be self-resonant, or they may include external coupled elements such as capacitors, inductors, switches, diodes, transistors, transformers, and the like. The magnetic resonators may include distributed and lumped capacitance and inductance. In general, the Q of the resonators will be determined by the Q'"'"'s of all the individual components of the resonator.
Because Q is proportional to inductance, L, resonators may be designed to increase L, within certain other constraints. One way to increase L, for example, is to use more than one turn of the conductor to form the inductor in the resonator. Design techniques and trade-offs may depend on the application, and a wide variety of structures, conductors, components, and resonant frequencies may be chosen in the design of high-Q magnetic resonators.
In the absence of significant absorption losses, the Q of the resonator may be determined primarily by the radiation losses, and given by, Qrad=ωL/Rrad, where Rrad is the radiative loss of the resonator and may depend on the size of the resonator relative to the frequency, ω, or wavelength, λ, of operation. For the magnetic resonators discussed above, radiative losses may scale as Rrad˜(x/λ)4 (characteristic of magnetic dipole radiation), where x is a characteristic dimension of the resonator, such as the radius of the inductive element shown in
Note too that the design of resonators for non-radiative wireless energy transfer differs from antennas designed for communication or far-field energy transmission purposes. Specifically, capacitively-loaded conductive loops may be used as resonant antennas (for example in cell phones), but those operate in the far-field regime where the radiation Q'"'"'s are intentionally designed to be small to make the antenna efficient at radiating energy. Such designs are not appropriate for the efficient near-field wireless energy transfer technique disclosed in this application.
The quality factor of a resonator including both radiative and absorption losses is Q=ωL/(Rabs+Rrad). Note that there may be a maximum Q value for a particular resonator and that resonators may be designed with special consideration given to the size of the resonator, the materials and elements used to construct the resonator, the operating frequency, the connection mechanisms, and the like, in order to achieve a high-Q resonator.
When the resonator is being described in terms of loss rates, the Q may be defined using the intrinsic decay rate, 2Γ, as described previously. The intrinsic decay rate is the rate at which an uncoupled and undriven resonator loses energy. For the magnetic resonators described above, the intrinsic loss rate may be given by Γ=(Rabs+Rrad)/2L, and the quality factor, Q, of the resonator is given by Q=ω/2Γ.
Note that a quality factor related only to a specific loss mechanism may be denoted as Qmechanism, if the resonator is not specified, or as Q1,mechanism, if the resonator is specified (e.g. resonator 1). For example, Q1,rad the quality factor for resonator 1 related to its radiation losses.
Electromagnetic Resonator Near-Fields
The high-Q electromagnetic resonators used in the near-field wireless energy transfer system disclosed here may be sub-wavelength objects. That is, the physical dimensions of the resonator may be much smaller than the wavelength corresponding to the resonant frequency. Sub-wavelength magnetic resonators may have most of the energy in the region surrounding the resonator stored in their magnetic near-fields, and these fields may also be described as stationary or non-propagating because they do not radiate away from the resonator. The extent of the near-field in the area surrounding the resonator is typically set by the wavelength, so it may extend well beyond the resonator itself for a sub-wavelength resonator. The limiting surface, where the field behavior changes from near-field behavior to far-field behavior may be called the “radiation caustic”.
The strength of the near-field is reduced the farther one gets away from the resonator. While the field strength of the resonator near-fields decays away from the resonator, the fields may still interact with objects brought into the general vicinity of the resonator. The degree to which the fields interact depends on a variety of factors, some of which may be controlled and designed, and some of which may not. The wireless energy transfer schemes described herein may be realized when the distance between coupled resonators is such that one resonator lies within the radiation caustic of the other.
The near-field profiles of the electromagnetic resonators may be similar to those commonly associated with dipole resonators or oscillators. Such field profiles may be described as omni-directional, meaning the magnitudes of the fields are non-zero in all directions away from the object.
Characteristic Size of an Electromagnetic Resonator
Spatially separated and/or offset magnetic resonators of sufficient Q may achieve efficient wireless energy transfer over distances that are much larger than have been seen in the prior art, even if the sizes and shapes of the resonator structures are different. Such resonators may also be operated to achieve more efficient energy transfer than was achievable with previous techniques over shorter range distances. We describe such resonators as being capable of mid-range energy transfer.
Mid-range distances may be defined as distances that are larger than the characteristic dimension of the smallest of the resonators involved in the transfer, where the distance is measured from the center of one resonator structure to the center of a spatially separated second resonator structure. In this definition, two-dimensional resonators are spatially separated when the areas circumscribed by their inductive elements do not intersect and three-dimensional resonators are spatially separated when their volumes do not intersect. A two-dimensional resonator is spatially separated from a three-dimensional resonator when the area circumscribed by the former is outside the volume of the latter.
In this inventive wireless energy transfer technique, energy may be exchanged efficiently over a wide range of distances, but the technique is distinguished by the ability to exchange useful energy for powering or recharging devices over mid-range distances and between resonators with different physical dimensions, components and orientations. Note that while k may be small in these circumstances, strong coupling and efficient energy transfer may be realized by using high-Q resonators to achieve a high U, U=k√{square root over (QsQd)}. That is, increases in Q may be used to at least partially overcome decreases in k, to maintain useful energy transfer efficiencies.
Note too that while the near-field of a single resonator may be described as omni-directional, the efficiency of the energy exchange between two resonators may depend on the relative position and orientation of the resonators. That is, the efficiency of the energy exchange may be maximized for particular relative orientations of the resonators. The sensitivity of the transfer efficiency to the relative position and orientation of two uncompensated resonators may be captured in the calculation of either k or κ. While coupling may be achieved between resonators that are offset and/or rotated relative to each other, the efficiency of the exchange may depend on the details of the positioning and on any feedback, tuning, and compensation techniques implemented during operation.
High-Q Magnetic Resonators
In the near-field regime of a sub-wavelength capacitively-loaded loop magnetic resonator (x<<λ), the resistances associated with a circular conducting loop inductor composed of N turns of wire whose radius is larger than the skin depth, are approximately Rabs=√{square root over (μoρω/2)}·Nx/a and Rrad=π/6·ηoN2 (ωx/c)4, where ρ is the resistivity of the conductor material and ηo≈120πΩ is the impedance of free space. The inductance, L, for such a N-turn loop is approximately N2 times the inductance of a single-turn loop given previously. The quality factor of such a resonator, Q=ωL/(Rabs+Rrad), is highest for a particular frequency determined by the system parameters (
Note that the formulas given above are approximate and intended to illustrate the functional dependence of Rabs, Rrad and L on the physical parameters of the structure. More accurate numerical calculations of these parameters that take into account deviations from the strict quasi-static limit, for example a non-uniform current/charge distribution along the conductor, may be useful for the precise design of a resonator structure.
Note that the absorptive losses may be minimized by using low loss conductors to form the inductive elements. The loss of the conductors may be minimized by using large surface area conductors such as conductive tubing, strapping, strips, machined objects, plates, and the like, by using specially designed conductors such as Litz wire, braided wires, wires of any cross-section, and other conductors with low proximity losses, in which case the frequency scaled behavior described above may be different, and by using low resistivity materials such as high-purity copper and silver, for example. One advantage of using conductive tubing as the conductor at higher operating frequencies is that it may be cheaper and lighter than a similar diameter solid conductor, and may have similar resistance because most of the current is traveling along the outer surface of the conductor owing to the skin effect.
To get a rough estimate of achievable resonator designs made from copper wire or copper tubing and appropriate for operation in the microwave regime, one may calculate the optimum Q and resonant frequency for a resonator composed of one circular inductive element (N=1) of copper wire (ρ=1.69·10−8 Ωm) with various cross sections. Then for an inductive element with characteristic size x=1 cm and conductor diameter a=1 mm, appropriate for a cell phone for example, the quality factor peaks at Q=1225 when f=380 MHz. For x=30 cm and a=2 mm, an inductive element size that might be appropriate for a laptop or a household robot, Q=1103 at f=17 MHz. For a larger source inductive element that might be located in the ceiling for example, x=1 m and a=4 mm, Q may be as high as Q=1315 at f=5 MHz. Note that a number of practical examples yield expected quality factors of Q≈1000-1500 at λ/x≈50-80. Measurements of a wider variety of coil shapes, sizes, materials and operating frequencies than described above show that Q'"'"'s>100 may be realized for a variety of magnetic resonator structures using commonly available materials.
As described above, the rate for energy transfer between two resonators of characteristic size x1 and x2, and separated by a distance D between their centers, may be given by κ. To give an example of how the defined parameters scale, consider the cell phone, laptop, and ceiling resonator examples from above, at three (3) distances; D/x=10, 8, 6. In the examples considered here, the source and device resonators are the same size, x1=x2, and shape, and are oriented as shown in
Inductive elements may be formed for use in high-Q magnetic resonators. We have demonstrated a variety of high-Q magnetic resonators based on copper conductors that are formed into inductive elements that enclose a surface. Inductive elements may be formed using a variety of conductors arranged in a variety of shapes, enclosing any size or shaped area, and they may be single turn or multiple turn elements. Drawings of exemplary inductive elements 900A-B are shown in
These conductors may be bent or formed into the desired size, shape, and number of turns. However, it may be difficult to accurately reproduce conductor shapes and sizes using manual techniques. In addition, it may be difficult to maintain uniform or desired center-to-center spacings between the conductor segments in adjacent turns of the inductive elements. Accurate or uniform spacing may be important in determining the self capacitance of the structure as well as any proximity effect induced increases in AC resistance, for example.
Molds may be used to replicate inductor elements for high-Q resonator designs. In addition, molds may be used to accurately shape conductors into any kind of shape without creating kinks, buckles or other potentially deleterious effects in the conductor. Molds may be used to form the inductor elements and then the inductor elements may be removed from the forms. Once removed, these inductive elements may be built into enclosures or devices that may house the high-Q magnetic resonator. The formed elements may also or instead remain in the mold used to form them.
The molds may be formed using standard CNC (computer numerical control) routing or milling tools or any other known techniques for cutting or forming grooves in blocks. The molds may also or instead be formed using machining techniques, injection molding techniques, casting techniques, pouring techniques, vacuum techniques, thermoforming techniques, cut-in-place techniques, compression forming techniques and the like.
The formed element may be removed from the mold or it may remain in the mold. The mold may be altered with the inductive element inside. The mold may be covered, machined, attached, painted and the like. The mold and conductor combination may be integrated into another housing, structure or device. The grooves cut into the molds may be any dimension and may be designed to form conducting tubing, wire, strapping, strips, blocks, and the like into the desired inductor shapes and sizes.
The inductive elements used in magnetic resonators may contain more than one loop and may spiral inward or outward or up or down or in some combination of directions. In general, the magnetic resonators may have a variety of shapes, sizes and number of turns and they may be composed of a variety of conducing materials.
The magnetic resonators may be free standing or they may be enclosed in an enclosure, container, sleeve or housing. The magnetic resonators may include the form used to make the inductive element. These various forms and enclosures may be composed of almost any kind of material. Low loss materials such as Teflon, REXOLITE, styrene, and the like may be preferable for some applications. These enclosures may contain fixtures that hold the inductive elements.
Magnetic resonators may be composed of self-resonant coils of copper wire or copper tubing. Magnetic resonators composed of self resonant conductive wire coils may include a wire of length l, and cross section radius a, wound into a helical coil of radius x, height h, and number of turns N, which may for example be characterized as N=√{square root over (l2−h2)}/2πx.
A magnetic resonator structure may be configured so that x is about 30 cm, h is about 20 cm, a is about 3 mm and N is about 5.25, and, during operation, a power source coupled to the magnetic resonator may drive the resonator at a resonant frequency, f, where f is about 10.6 MHz. Where x is about 30 cm, h is about 20 cm, a is about 1 cm and N is about 4, the resonator may be driven at a frequency, f, where f is about 13.4 MHz. Where x is about 10 cm, h is about 3 cm, a is about 2 mm and N is about 6, the resonator may be driven at a frequency, f, where f is about 21.4 MHz.
High-Q inductive elements may be designed using printed circuit board traces. Printed circuit board traces may have a variety of advantages compared to mechanically formed inductive elements including that they may be accurately reproduced and easily integrated using established printed circuit board fabrication techniques, that their AC resistance may be lowered using custom designed conductor traces, and that the cost of mass-producing them may be significantly reduced.
High-Q inductive elements may be fabricated using standard PCB techniques on any PCB material such as FR-4 (epoxy E-glass), multi-functional epoxy, high performance epoxy, bismalaimide triazine/epoxy, polyimide, Cyanate Ester, polytetraflouroethylene (Teflon), FR-2, FR-3, CEM-1, CEM-2, Rogers, Resolute, and the like. The conductor traces may be formed on printed circuit board materials with lower loss tangents.
The conducting traces may be composed of copper, silver, gold, aluminum, nickel and the like, and they may be composed of paints, inks, or other cured materials. The circuit board may be flexible and it may be a flex-circuit. The conducting traces may be formed by chemical deposition, etching, lithography, spray deposition, cutting, and the like. The conducting traces may be applied to form the desired patterns and they may be formed using crystal and structure growth techniques.
The dimensions of the conducting traces, as well as the number of layers containing conducting traces, the position, size and shape of those traces and the architecture for interconnecting them may be designed to achieve or optimize certain system specifications such as resonator Q, Q(p), resonator size, resonator material and fabrication costs, U, U(p), and the like.
As an example, a three-turn high-Q inductive element 1001A was fabricated on a four-layer printed circuit board using the rectangular copper trace pattern as shown in
As another example, a two-turn inductor 1001B was fabricated on a four-layer printed circuit board using the rectangular copper trace pattern shown in
The inductive elements may be formed using magnetic materials of any size, shape thickness, and the like, and of materials with a wide range of permeability and loss values. These magnetic materials may be solid blocks, they may enclose hollow volumes, they may be formed from many smaller pieces of magnetic material tiled and or stacked together, and they may be integrated with conducting sheets or enclosures made from highly conducting materials. Wires may be wrapped around the magnetic materials to generate the magnetic near-field. These wires may be wrapped around one or more than one axis of the structure. Multiple wires may be wrapped around the magnetic materials and combined in parallel, or in series, or via a switch to form customized near-field patterns.
The magnetic resonator may include 15 turns of Litz wire wound around a 19.2 cm×10 cm×5 mm tiled block of 3F3 ferrite material. The Litz wire may be wound around the ferrite material in any direction or combination of directions to achieve the desire resonator performance. The number of turns of wire, the spacing between the turns, the type of wire, the size and shape of the magnetic materials and the type of magnetic material are all design parameters that may be varied or optimized for different application scenarios.
High-Q Magnetic Resonators Using Magnetic Material Structures
It may be possible to use magnetic materials assembled to form an open magnetic circuit, albeit one with an air gap on the order of the size of the whole structure, to realize a magnetic resonator structure. In these structures, high conductivity materials are wound around a structure made from magnetic material to form the inductive element of the magnetic resonator. Capacitive elements may be connected to the high conductivity materials, with the resonant frequency then determined as described above. These magnetic resonators have their dipole moment in the plane of the two dimensional resonator structures, rather than perpendicular to it, as is the case for the capacitively-loaded inductor loop resonators.
A diagram of a single planar resonator structure is shown in
The geometry and the coupling orientations of the described planar resonators may be preferable for some applications. The planar or flat resonator shape may be easier to integrate into many electronic devices that are relatively flat and planar. The planar resonators may be integrated into the whole back or side of a device without requiring a change in geometry of the device. Due to the flat shape of many devices, the natural position of the devices when placed on a surface is to lay with their largest dimension being parallel to the surface they are placed on. A planar resonator integrated into a flat device is naturally parallel to the plane of the surface and is in a favorable coupling orientation relative to the resonators of other devices or planar resonator sources placed on a flat surface.
As mentioned, the geometry of the planar resonators may allow easier integration into devices. Their low profile may allow a resonator to be integrated into or as part of a complete side of a device. When a whole side of a device is covered by the resonator, magnetic flux can flow through the resonator core without being obstructed by lossy material that may be part of the device or device circuitry.
The core of the planar resonator structure may be of a variety of shapes and thicknesses and may be flat or planar such that the minimum dimension does not exceed 30% of the largest dimension of the structure. The core may have complex geometries and may have indentations, notches, ridges, and the like. Geometric enhancements may be used to reduce the coupling dependence on orientation and they may be used to facilitate integration into devices, packaging, packages, enclosures, covers, skins, and the like. Two exemplary variations of core geometries are shown in
The shape and dimensions of the core may be further dictated by the dimensions and characteristics of the device that they are integrated into. The core material may curve to follow the contours of the device, or may require non-symmetric notches or cutouts to allow clearance for parts of the device. The core structure may be a single monolithic piece of magnetic material or may be composed of a plurality of tiles, blocks, or pieces that are arranged together to form the larger structure. The different layers, tiles, blocks, or pieces of the structure may be of similar or may be of different materials. It may be desirable to use materials with different magnetic permeability in different locations of the structure. Core structures with different magnetic permeability may be useful for guiding the magnetic flux, improving coupling, and affecting the shape or extent of the active area of a system.
The conductor of the planar resonator structure may be wound at least once around the core. In certain circumstances, it may be preferred to wind at least three loops. The conductor can be any good conductor including conducting wire, Litz wire, conducting tubing, sheets, strips, gels, inks, traces and the like.
The size, shape, or dimensions of the active area of source may be further enhanced, altered, or modified with the use of materials that block, shield, or guide magnetic fields. To create non-symmetric active area around a source once side of the source may be covered with a magnetic shield to reduce the strength of the magnetic fields in a specific direction. The shield may be a conductor or a layered combination of conductor and magnetic material which can be used to guide magnetic fields away from a specific direction. Structures composed of layers of conductors and magnetic materials may be used to reduce energy losses that may occur due to shielding of the source.
The plurality of planar resonators may be integrated or combined into one planar resonator structure. A conductor or conductors may be wound around a core structure such that the loops formed by the two conductors are not coaxial. An example of such a structure is shown in
Non-uniform or asymmetric field profiles around the resonator comprising a plurality of conductor loops may be generated by driving some conductor loops with non-identical parameters. Some conductor loops of a source resonator with a plurality of conductor loops may be driven by a power source with a different frequency, voltage, power level, duty cycle, and the like all of which may be used to affect the strength of the magnetic field generated by each conductor.
The planar resonator structures may be combined with a capacitively-loaded inductor resonator coil to provide an omni-directional active area all around, including above and below the source while maintaining a flat resonator structure. As shown in
The planar resonator structures may be enclosed in magnetically permeable packaging or integrated into other devices. The planar profile of the resonators within a single, common plane allows packaging and integration into flat devices. A diagram illustrating the application of the resonators is shown in
Another diagram illustrating a possible use of a power transfer system using the planar resonator structures is shown in
The source may include a display or other visual, auditory, or vibration indicators to show the direction of charging devices or what devices are being charged, error or problems with charging, power levels, charging time, and the like.
The source resonators and circuitry may be integrated into any number of other devices. The source may be integrated into devices such as clocks, keyboards, monitors, picture frames, and the like. For example, a keyboard integrated with the planar resonators and appropriate power and control circuitry may be used as a source for devices placed around the keyboard such as computer mice, webcams, mobile handsets, and the like without occupying any additional desk space.
While the planar resonator structures have been described in the context of mobile devices it should be clear to those skilled in the art that a flat planar source for wireless power transfer with an active area that extends beyond its physical dimensions has many other consumer and industrial applications. The structures and configuration may be useful for a large number of applications where electronic or electric devices and a power source are typically located, positioned, or manipulated in substantially the same plane and alignment. Some of the possible application scenarios include devices on walls, floor, ceilings or any other substantially planar surfaces.
Flat source resonators may be integrated into a picture frame or hung on a wall thereby providing an active area within the plane of the wall where other electronic devices such as digital picture frames, televisions, lights, and the like can be mounted and powered without wires. Planar resonators may be integrated into a floor resulting in an energized floor or active area on the floor on which devices can be placed to receive power. Audio speakers, lamps, heaters, and the like can be placed within the active are and receive power wirelessly.
The planar resonator may have additional components coupled to the conductor. Components such as capacitors, inductors, resistors, diodes, and the like may be coupled to the conductor and may be used to adjust or tune the resonant frequency and the impedance matching for the resonators.
A planar resonator structure of the type described above and shown in
In addition to utilizing magnetic materials to realize a structure with properties similar to the inductive element in the magnetic resonators, it may be possible to use a combination of good conductor materials and magnetic material to realize such inductive structures.
A structure may include a high-conductivity sheet of material covered on one side by a layer of magnetic material. The layered structure may instead be applied conformally to an electronic device, so that parts of the device may be covered by the high-conductivity and magnetic material layers, while other parts that need to be easily accessed (such as buttons or screens) may be left uncovered. The structure may also or instead include only layers or bulk pieces of magnetic material. Thus, a magnetic resonator may be incorporated into an existing device without significantly interfering with its existing functions and with little or no need for extensive redesign. Moreover, the layers of good conductor and/or magnetic material may be made thin enough (of the order of a millimeter or less) that they would add little extra weight and volume to the completed device. An oscillating current applied to a length of conductor wound around the structure, as shown by the square loop in the center of the structure in
Quality Factor of the Structure
A structure of the type described above may be created with a quality factor, Q, of the order of 1,000 or higher. This high-Q is possible even if the losses in the magnetic material are high, if the fraction of magnetic energy within the magnetic material is small compared to the total magnetic energy associated with the object. For structures composed of layers conducting materials and magnetic materials, the losses in the conducting materials may be reduced by the presence of the magnetic materials as described previously. In structures where the magnetic material layer'"'"'s thickness is of the order of 1/100 of the largest dimension of the system (e.g., the magnetic material may be of the order of 1 mm thick, while the area of the structure is of the order of 10 cm×10 cm), and the relative permeability is of the order of 1,000, it is possible to make the fraction of magnetic energy contained within the magnetic material only a few hundredths of the total magnetic energy associated with the object or resonator. To see how that comes about, note that the expression for the magnetic energy contained in a volume is Um=∫VdrB(r)2/(2μrμ0), so as long as B (rather than H) is the main field conserved across the magnetic material-air interface (which is typically the case in open magnetic circuits), the fraction of magnetic energy contained in the high-μr region may be significantly reduced compared to what it is in air.
If the fraction of magnetic energy in the magnetic material is denoted by frac, and the loss tangent of the material is tan δ, then the Q of the resonator, assuming the magnetic material is the only source of losses, is Q=1/(frac×tan δ). Thus, even for loss tangents as high as 0.1, it is possible to achieve Q'"'"'s of the order of 1,000 for these types of resonator structures.
If the structure is driven with N turns of wire wound around it, the losses in the excitation inductor loop can be ignored if N is sufficiently high.
Electromagnetic Resonators Interacting with Other Objects
For electromagnetic resonators, extrinsic loss mechanisms that perturb the intrinsic Q may include absorption losses inside the materials of nearby extraneous objects and radiation losses related to scattering of the resonant fields from nearby extraneous objects. Absorption losses may be associated with materials that, over the frequency range of interest, have non-zero, but finite, conductivity, σ, (or equivalently a non-zero and finite imaginary part of the dielectric permittivity), such that electromagnetic fields can penetrate it and induce currents in it, which then dissipate energy through resistive losses. An object may be described as lossy if it at least partly includes lossy materials.
Consider an object including a homogeneous isotropic material of conductivity, σ and magnetic permeability, μ. The penetration depth of electromagnetic fields inside this object is given by the skin depth, δ=√{square root over (2/ωμσ)}. The power dissipated inside the object, Pd, can be determined from Pd=∫Vdrσ|E|2=∫Vdr|J|2/σ where we made use of Ohm'"'"'s law, J=σE, and where E is the electric field and J is the current density.
If over the frequency range of interest, the conductivity, σ, of the material that composes the object is low enough that the material'"'"'s skin depth, δ, may be considered long, (i.e. δ is longer than the objects'"'"' characteristic size, or δ is longer than the characteristic size of the portion of the object that is lossy) then the electromagnetic fields, E and H, where H is the magnetic field, may penetrate significantly into the object. Then, these finite-valued fields may give rise to a dissipated power that scales as Pd˜σVol where Vol is the volume of the object that is lossy and
is the spatial average of the electric-field squared, in the volume under consideration. Therefore, in the low-conductivity limit, the dissipated power scales proportionally to the conductivity and goes to zero in the limit of a non-conducting (purely dielectric) material.
If over the frequency range of interest, the conductivity, σ, of the material that composes the object is high enough that the material'"'"'s skin depth may be considered short, then the electromagnetic fields, E and H, may penetrate only a short distance into the object (namely they stay close to the ‘skin’ of the material, where δ is smaller than the characteristic thickness of the portion of the object that is lossy). In this case, the currents induced inside the material may be concentrated very close to the material surface, approximately within a skin depth, and their magnitude may be approximated by the product of a surface current density (mostly determined by the shape of the incident electromagnetic fields and, as long as the thickness of the conductor is much larger than the skin-depth, independent of frequency and conductivity to first order) K(x, y) (where x and y are coordinates parameterizing the surface) and a function decaying exponentially into the surface: exp(−z/δ)/δ (where z denotes the coordinate locally normal to the surface): J(x, y, z)=K(x, y)exp(−z/δ)/δ. Then, the dissipated power, Pd, may be estimated by,
Pd=vdr(r)|2/σ≃(sdxdy|K(x,y)|2)((∞0dz exp(2z/δ)/(σδ2))=√{square root over (μω/8σ)}(sdxdy|K(x,y)|2)
Therefore, in the high-conductivity limit, the dissipated power scales inverse proportionally to the square-root of the conductivity and goes to zero in the limit of a perfectly-conducting material.
If over the frequency range of interest, the conductivity, σ, of the material that composes the object is finite, then the material'"'"'s skin depth, δ, may penetrate some distance into the object and some amount of power may be dissipated inside the object, depending also on the size of the object and the strength of the electromagnetic fields. This description can be generalized to also describe the general case of an object including multiple different materials with different properties and conductivities, such as an object with an arbitrary inhomogeneous and anisotropic distribution of the conductivity inside the object.
Note that the magnitude of the loss mechanisms described above may depend on the location and orientation of the extraneous objects relative to the resonator fields as well as the material composition of the extraneous objects. For example, high-conductivity materials may shift the resonant frequency of a resonator and detune it from other resonant objects. This frequency shift may be fixed by applying a feedback mechanism to a resonator that corrects its frequency, such as through changes in the inductance and/or capacitance of the resonator. These changes may be realized using variable capacitors and inductors, in some cases achieved by changes in the geometry of components in the resonators. Other novel tuning mechanisms, described below, may also be used to change the resonator frequency.
Where external losses are high, the perturbed Q may be low and steps may be taken to limit the absorption of resonator energy inside such extraneous objects and materials. Because of the functional dependence of the dissipated power on the strength of the electric and magnetic fields, one might optimize system performance by designing a system so that the desired coupling is achieved with shorter evanescent resonant field tails at the source resonator and longer at the device resonator, so that the perturbed Q of the source in the presence of other objects is optimized (or vice versa if the perturbed Q of the device needs to be optimized).
Note that many common extraneous materials and objects such as people, animals, plants, building materials, and the like, may have low conductivities and therefore may have little impact on the wireless energy transfer scheme disclosed here. An important fact related to the magnetic resonator designs we describe is that their electric fields may be confined primarily within the resonator structure itself, so it should be possible to operate within the commonly accepted guidelines for human safety while providing wireless power exchange over mid range distances.
Electromagnetic Resonators with Reduced Interactions
One frequency range of interest for near-field wireless power transmission is between 10 kHz and 100 MHz. In this frequency range, a large variety of ordinary non-metallic materials, such as for example several types of wood and plastic may have relatively low conductivity, such that only small amounts of power may be dissipated inside them. In addition, materials with low loss tangents, tan Δ, where tan Δ=∈″/∈′, and ∈″ and ∈′ are the imaginary and real parts of the permittivity respectively, may also have only small amounts of power dissipated inside them. Metallic materials, such as copper, silver, gold, and the like, with relatively high conductivity, may also have little power dissipated in them, because electromagnetic fields are not able to significantly penetrate these materials, as discussed earlier. These very high and very low conductivity materials, and low loss tangent materials and objects may have a negligible impact on the losses of a magnetic resonator.
However, in the frequency range of interest, there are materials and objects such as some electronic circuits and some lower-conductivity metals, which may have moderate (in general inhomogeneous and anisotropic) conductivity, and/or moderate to high loss tangents, and which may have relatively high dissipative losses. Relatively larger amounts of power may be dissipated inside them. These materials and objects may dissipate enough energy to reduce Q(p) by non-trivial amounts, and may be referred to as “lossy objects”.
One way to reduce the impact of lossy materials on the Q(p) of a resonator is to use high-conductivity materials to shape the resonator fields such that they avoid the lossy objects. The process of using high-conductivity materials to tailor electromagnetic fields so that they avoid lossy objects in their vicinity may be understood by visualizing high-conductivity materials as materials that deflect or reshape the fields. This picture is qualitatively correct as long as the thickness of the conductor is larger than the skin-depth because the boundary conditions for electromagnetic fields at the surface of a good conductor force the electric field to be nearly completely perpendicular to, and the magnetic field to be nearly completely tangential to, the conductor surface. Therefore, a perpendicular magnetic field or a tangential electric field will be “deflected away” from the conducting surface. Furthermore, even a tangential magnetic field or a perpendicular electric field may be forced to decrease in magnitude on one side and/or in particular locations of the conducting surface, depending on the relative position of the sources of the fields and the conductive surface.
As an example,
A similar effect is observed even if only one conducting surface, above or below, the dielectric disk, is used. If the dielectric disk is thin, the fact that the electric field is essentially zero at the surface, and continuous and smooth close to it, means that the electric field is very low everywhere close to the surface (i.e. within the dielectric disk). A single surface implementation for deflecting resonator fields away from lossy objects may be preferred for applications where one is not allowed to cover both sides of the lossy material or object (e.g. an LCD screen). Note that even a very thin surface of conducting material, on the order of a few skin-depths, may be sufficient (the skin depth in pure copper at 6.78 MHz is ˜20 μm, and at 250 kHz is ˜100 μm) to significantly improve the Q(p) of a resonator in the presence of lossy materials.
Lossy extraneous materials and objects may be parts of an apparatus, in which a high-Q resonator is to be integrated. The dissipation of energy in these lossy materials and objects may be reduced by a number of techniques including:
- by positioning the lossy materials and objects away from the resonator, or, in special positions and orientations relative to the resonator.
- by using a high conductivity material or structure to partly or entirely cover lossy materials and objects in the vicinity of a resonator
- by placing a closed surface (such as a sheet or a mesh) of high-conductivity material around a lossy object to completely cover the lossy object and shape the resonator fields such that they avoid the lossy object.
- by placing a surface (such as a sheet or a mesh) of a high-conductivity material around only a portion of a lossy object, such as along the top, the bottom, along the side, and the like, of an object or material.
- by placing even a single surface (such as a sheet or a mesh) of high-conductivity material above or below or on one side of a lossy object to reduce the strength of the fields at the location of the lossy object.
Extraneous losses may be reduced, but may not be completely eliminated, by placing a single surface of high-conductivity material above, below, on the side, and the like, of a lossy object or material. An example is shown in
A single surface of high-conductivity material may be used to avoid objects that cannot or should not be covered from both sides (e.g. LCD or plasma screens). Such lossy objects may be avoided using optically transparent conductors. High-conductivity optically opaque materials may instead be placed on only a portion of the lossy object, instead of, or in addition to, optically transparent conductors. The adequacy of single-sided vs. multi-sided covering implementations, and the design trade-offs inherent therein may depend on the details of the wireless energy transfer scenario and the properties of the lossy materials and objects.
Below we describe an example using high-conductivity surfaces to improve the Q-insensitivity, Θ(p), of an integrated magnetic resonator used in a wireless energy-transfer system.
In a completely wireless projector example, covering the network/video adapter card with a thin copper pocket (a folded sheet of copper that covered the top and the bottom of the wireless network/video adapter card, but not the communication antenna) improved the Q(integrated) of the magnetic resonator to a Q(integrated+copper pocket) of approximately 444. In other words, most of the reduction in Q(integrated) due to the perturbation caused by the extraneous network/video adapter card could be eliminated using a copper pocket to deflect the resonator fields away from the lossy materials.
In another completely wireless projector example, covering the network/video adapter card with a single copper sheet placed beneath the card provided a Q(integrated+copper sheet) approximately equal to Q(integrated+copper pocket). In that example, the high perturbed Q of the system could be maintained with a single high-conductivity sheet used to deflect the resonator fields away from the lossy adapter card.
It may be advantageous to position or orient lossy materials or objects, which are part of an apparatus including a high-Q electromagnetic resonator, in places where the fields produced by the resonator are relatively weak, so that little or no power may be dissipated in these objects and so that the Q-insensitivity, Θ(p), may be large. As was shown earlier, materials of different conductivity may respond differently to electric versus magnetic fields. Therefore, according to the conductivity of the extraneous object, the positioning technique may be specialized to one or the other field.
In a demonstration example, a magnetic resonator was formed using a three-turn conductor loop, arranged to enclose a square surface (with rounded corners), and a capacitor network. The Q of the resonator was approximately 619 at the designed operating resonant frequency of 6.78 MHz. The perturbed Q of this resonator depended on the placement of the perturbing object, in this case a pocket projector, relative to the resonator. When the perturbing projector was located inside the inductor loop and at its center or on top of the inductor wire turns, Q(projector) was approximately 96, lower than when the perturbing projector was placed outside of the resonator, in which case Q(projector) was approximately 513. These measurements support the analysis that shows the fields inside the inductor loop may be larger than those outside it, so lossy objects placed inside such a loop inductor may yield lower perturbed Q'"'"'s for the system than when the lossy object is placed outside the loop inductor. Depending on the resonator designs and the material composition and orientation of the lossy object, the arrangement shown in
High-Q resonators may be integrated inside an apparatus. Extraneous materials and objects of high dielectric permittivity, magnetic permeability, or electric conductivity may be part of the apparatus into which a high-Q resonator is to be integrated. For these extraneous materials and objects in the vicinity of a high-Q electromagnetic resonator, depending on their size, position and orientation relative to the resonator, the resonator field-profile may be distorted and deviate significantly from the original unperturbed field-profile of the resonator. Such a distortion of the unperturbed fields of the resonator may significantly decrease the Q to a lower Q(p), even if the extraneous objects and materials are lossless.
It may be advantageous to position high-conductivity objects, which are part of an apparatus including a high-Q electromagnetic resonator, at orientations such that the surfaces of these objects are, as much as possible, perpendicular to the electric field lines produced by the unperturbed resonator and parallel to the magnetic field lines produced by the unperturbed resonator, thus distorting the resonant field profiles by the smallest amount possible. Other common objects that may be positioned perpendicular to the plane of a magnetic resonator loop include screens (LCD, plasma, etc), batteries, cases, connectors, radiative antennas, and the like. The Q-insensitivity, Θ(p), of the resonator may be much larger than if the objects were positioned at a different orientation with respect to the resonator fields.
Lossy extraneous materials and objects, which are not part of the integrated apparatus including a high-Q resonator, may be located or brought in the vicinity of the resonator, for example, during the use of the apparatus. It may be advantageous in certain circumstances to use high conductivity materials to tailor the resonator fields so that they avoid the regions where lossy extraneous objects may be located or introduced to reduce power dissipation in these materials and objects and to increase Q-insensitivity, Θ(p). An example is shown in
Note that a high-conductivity surface brought in the vicinity of a resonator to reshape the fields may also lead to Q(cond. surface)<Q. The reduction in the perturbed Q may be due to the dissipation of energy inside the lossy conductor or to the distortion of the unperturbed resonator field profiles associated with matching the field boundary conditions at the surface of the conductor. Therefore, while a high-conductivity surface may be used to reduce the extraneous losses due to dissipation inside an extraneous lossy object, in some cases, especially in some of those where this is achieved by significantly reshaping the electromagnetic fields, using such a high-conductivity surface so that the fields avoid the lossy object may result effectively in Q(p+cond. surface)<Q(p) rather than the desired result Q(p+cond. surface)>Q(p).
As described above, in the presence of loss inducing objects, the perturbed quality factor of a magnetic resonator may be improved if the electromagnetic fields associated with the magnetic resonator are reshaped to avoid the loss inducing objects. Another way to reshape the unperturbed resonator fields is to use high permeability materials to completely or partially enclose or cover the loss inducing objects, thereby reducing the interaction of the magnetic field with the loss inducing objects.
Magnetic field shielding has been described previously, for example in Electrodynamics 3rd Ed., Jackson, pp. 201-203. There, a spherical shell of magnetically permeable material was shown to shield its interior from external magnetic fields. For example, if a shell of inner radius a, outer radius b, and relative permeability, μr, is placed in an initially uniform magnetic field H0, then the field inside the shell will have a constant magnitude, 9μrH0/[(2μr+1)(μr+2)−2(a/b)3(μr−1)2], which tends to 9H0/2μr(1−(a/b)3) if μr>>1. This result shows that an incident magnetic field (but not necessarily an incident electric field) may be greatly attenuated inside the shell, even if the shell is quite thin, provided the magnetic permeability is high enough. It may be advantageous in certain circumstances to use high permeability materials to partly or entirely cover lossy materials and objects so that they are avoided by the resonator magnetic fields and so that little or no power is dissipated in these materials and objects. In such an approach, the Q-insensitivity, Θ(p), may be larger than if the materials and objects were not covered, possibly larger than 1.
It may be desirable to keep both the electric and magnetic fields away from loss inducing objects. As described above, one way to shape the fields in such a manner is to use high-conductivity surfaces to either completely or partially enclose or cover the loss inducing objects. A layer of magnetically permeable material, also referred to as magnetic material, (any material or meta-material having a non-trivial magnetic permeability), may be placed on or around the high-conductivity surfaces. The additional layer of magnetic material may present a lower reluctance path (compared to free space) for the deflected magnetic field to follow and may partially shield the electric conductor underneath it from the incident magnetic flux. This arrangement may reduce the losses due to induced currents in the high-conductivity surface. Under some circumstances the lower reluctance path presented by the magnetic material may improve the perturbed Q of the structure.
This high-conductivity enclosure may increase the perturbing Q of the lossy objects and therefore the overall perturbed Q of the system, but the perturbed Q may still be less than the unperturbed Q because of induced losses in the conducting surface and changes to the profile of the electromagnetic fields. Decreases in the perturbed Q associated with the high-conductivity enclosure may be at least partially recovered by including a layer of magnetic material along the outer surface or surfaces of the high-conductivity enclosure.
Mathematical models were used to simulate a high-conductivity enclosure made of copper and shaped like a 20 cm diameter by 2 cm high cylindrical disk placed within an area circumscribed by a magnetic resonator whose inductive element was a single-turn wire loop with loop radius r=11 cm and wire radius a=1 mm. Simulations for an applied 6.78 MHz electromagnetic field suggest that the perturbing quality factor of this high-conductivity enclosure, δQ(enclosure), is 1,870. When the high-conductivity enclosure was modified to include a 0.25 cm-thick layer of magnetic material with real relative permeability, μr′=40, and imaginary relative permeability, μr″=10−2, simulations suggest the perturbing quality factor is increased to δQ(enclosure+magnetic material)=5,060.
The improvement in performance due to the addition of thin layers of magnetic material 2702 may be even more dramatic if the high-conductivity enclosure fills a larger portion of the area circumscribed by the resonator'"'"'s loop inductor 2704. In the example above, if the radius of the inductor loop 2704 is reduced so that it is only 3 mm away from the surface of the high-conductivity enclosure, the perturbing quality factor may be improved from 670 (conducting enclosure only) to 2,730 (conducting enclosure with a thin layer of magnetic material) by the addition of a thin layer of magnetic material 2702 around the outside of the enclosure.
The resonator structure may be designed to have highly confined electric fields, using shielding, or distributed capacitors, for example, which may yield high, even when the resonator is very close to materials that would typically induce loss.
Coupled Electromagnetic Resonators
The efficiency of energy transfer between two resonators may be determined by the strong-coupling figure-of-merit, U=κ/√{square root over (ΓsΓd)}=(2κ/√{square root over (ωsωd)})√{square root over (QsQd)}. In magnetic resonator implementations the coupling factor between the two resonators may be related to the inductance of the inductive elements in each of the resonators, L1 and L2, and the mutual inductance, M, between them by κ12=ωM/2√{square root over (L1L2)}. Note that this expression assumes there is negligible coupling through electric-dipole coupling. For capacitively-loaded inductor loop resonators where the inductor loops are formed by circular conducting loops with N turns, separated by a distance D, and oriented as shown in
For electromagnetic resonators, if the two resonators include conducting parts, the coupling mechanism may be that currents are induced on one resonator due to electric and magnetic fields generated from the other. The coupling factor may be proportional to the flux of the magnetic field produced from the high-Q inductive element in one resonator crossing a closed area of the high-Q inductive element of the second resonator.
Coupled Electromagnetic Resonators with Reduced Interactions
As described earlier, a high-conductivity material surface may be used to shape resonator fields such that they avoid lossy objects, p, in the vicinity of a resonator, thereby reducing the overall extraneous losses and maintaining a high Q-insensitivity Θ(p+cond. surface) of the resonator. However, such a surface may also lead to a perturbed coupling factor, k(p+cond. surface), between resonators that is smaller than the perturbed coupling factor, k(p) and depends on the size, position, and orientation of the high-conductivity material relative to the resonators. For example, if high-conductivity materials are placed in the plane and within the area circumscribed by the inductive element of at least one of the magnetic resonators in a wireless energy transfer system, some of the magnetic flux through the area of the resonator, mediating the coupling, may be blocked and k may be reduced.
Consider again the example of
One may use high-conductivity material structures, either alone, or combined with magnetic materials to optimize perturbed quality factors, perturbed coupling factors, or perturbed efficiencies.
Consider the example of
Where the high-conductivity surface below the lossy object covers the entire area of the inductor loop resonator (As=A), k12(object+cond. surface) may approach zero, because little flux is allowed to cross the inductor loop, so U12(object+cond. surface) may approach zero. For intermediate sizes of the high-conductivity surface, the suppression of extrinsic losses and the associated Q-insensitivity, Θ1(object+cond. surface), may be large enough compared to Θ1(object), while the reduction in coupling may not be significant and the associated k-insensitivity, β12(object+cond. surface), may be not much smaller than β12(object), so that the overall U12(object+cond. surface) may be increased compared to U12(object). The optimal degree of avoiding of extraneous lossy objects via high-conductivity surfaces in a system of wireless energy transfer may depend on the details of the system configuration and the application.
We describe using high-conductivity materials to either completely or partially enclose or cover loss inducing objects in the vicinity of high-Q resonators as one potential method to achieve high perturbed Q'"'"'s for a system. However, using a good conductor alone to cover the objects may reduce the coupling of the resonators as described above, thereby reducing the efficiency of wireless power transfer. As the area of the conducting surface approaches the area of the magnetic resonator, for example, the perturbed coupling factor, k(p), may approach zero, making the use of the conducting surface incompatible with efficient wireless power transfer.
One approach to addressing the aforementioned problem is to place a layer of magnetic material around the high-conductivity materials because the additional layer of permeable material may present a lower reluctance path (compared to free space) for the deflected magnetic field to follow and may partially shield the electric conductor underneath it from incident magnetic flux. Under some circumstances the lower reluctance path presented by the magnetic material may improve the electromagnetic coupling of the resonator to other resonators. Decreases in the perturbed coupling factor associated with using conducting materials to tailor resonator fields so that they avoid lossy objects in and around high-Q magnetic resonators may be at least partially recovered by including a layer of magnetic material along the outer surface or surfaces of the conducting materials. The magnetic materials may increase the perturbed coupling factor relative to its initial unperturbed value.
Note that the simulation results in
As described above,
Magnetic materials may be placed within the area circumscribed by the magnetic resonator to increase the coupling in wireless energy transfer systems. Consider a solid sphere of a magnetic material with relative permeability, μr, placed in an initially uniform magnetic field. In this example, the lower reluctance path offered by the magnetic material may cause the magnetic field to concentrate in the volume of the sphere. We find that the magnetic flux through the area circumscribed by the equator of the sphere is enhanced by a factor of 3μr/(μr+2), by the addition of the magnetic material. If μr>>1, this enhancement factor may be close to 3.
One can also show that the dipole moment of a system comprising the magnetic sphere circumscribed by the inductive element in a magnetic resonator would have its magnetic dipole enhanced by the same factor. Thus, the magnetic sphere with high permeability practically triples the dipole magnetic coupling of the resonator. It is possible to keep most of this increase in coupling if we use a spherical shell of magnetic material with inner radius a, and outer radius b, even if this shell is on top of block or enclosure made from highly conducting materials. In this case, the enhancement in the flux through the equator is
For μr=1,000 and (a/b)=0.99, this enhancement factor is still 2.73, so it possible to significantly improve the coupling even with thin layers of magnetic material.
As described above, structures containing magnetic materials may be used to realize magnetic resonators.
Electromagnetic Resonators and Impedance Matching
Impedance Matching Architectures for Low-Loss Inductive Elements
For purposes of the present discussion, an inductive element may be any coil or loop structure (the ‘loop’) of any conducting material, with or without a (gapped or ungapped) core made of magnetic material, which may also be coupled inductively or in any other contactless way to other systems. The element is inductive because its impedance, including both the impedance of the loop and the so-called ‘reflected’ impedances of any potentially coupled systems, has positive reactance, X, and resistance, R.
Consider an external circuit, such as a driving circuit or a driven load or a transmission line, to which an inductive element may be connected. The external circuit (e.g. a driving circuit) may be delivering power to the inductive element and the inductive element may be delivering power to the external circuit (e.g. a driven load). The efficiency and amount of power delivered between the inductive element and the external circuit at a desired frequency may depend on the impedance of the inductive element relative to the properties of the external circuit. Impedance-matching networks and external circuit control techniques may be used to regulate the power delivery between the external circuit and the inductive element, at a desired frequency, f.
The external circuit may be a driving circuit configured to form a amplifier of class A, B, C, D, DE, E, F and the like, and may deliver power at maximum efficiency (namely with minimum losses within the driving circuit) when it is driving a resonant network with specific impedance Zo*, where Zo may be complex and * denotes complex conjugation. The external circuit may be a driven load configured to form a rectifier of class A, B, C, D, DE, E, F and the like, and may receive power at maximum efficiency (namely with minimum losses within the driven load) when it is driven by a resonant network with specific impedance Zo*, where Zo may be complex. The external circuit may be a transmission line with characteristic impedance, Zo, and may exchange power at maximum efficiency (namely with zero reflections) when connected to an impedance Zo*. We will call the characteristic impedance Zo of an external circuit the complex conjugate of the impedance that may be connected to it for power exchange at maximum efficiency.
Typically the impedance of an inductive element, R+jX, may be much different from Zo*. For example, if the inductive element has low loss (a high X/R), its resistance, R, may be much lower than the real part of the characteristic impedance, Z0, of the external circuit. Furthermore, an inductive element by itself may not be a resonant network. An impedance-matching network connected to an inductive element may typically create a resonant network, whose impedance may be regulated.
Therefore, an impedance-matching network may be designed to maximize the efficiency of the power delivered between the external circuit and the inductive element (including the reflected impedances of any coupled systems). The efficiency of delivered power may be maximized by matching the impedance of the combination of an impedance-matching network and an inductive element to the characteristic impedance of an external circuit (or transmission line) at the desired frequency.
An impedance-matching network may be designed to deliver a specified amount of power between the external circuit and the inductive element (including the reflected impedances of any coupled systems). The delivered power may be determined by adjusting the complex ratio of the impedance of the combination of the impedance-matching network and the inductive element to the impedance of the external circuit (or transmission line) at the desired frequency.
Impedance-matching networks connected to inductive elements may create magnetic resonators. For some applications, such as wireless power transmission using strongly-coupled magnetic resonators, a high Q may be desired for the resonators. Therefore, the inductive ele