Wireless power transfer systems with shield openings
First Claim
1. An apparatus for wireless power transfer, the apparatus comprising:
- a plurality of adjacent magnetic elements positioned in a plane and defining a gap;
a coil comprising one or more loops of conductive material positioned, at least in part, on a first side of the plane and on both sides of the gap; and
a conductive shield positioned on a second side of the plane and comprising an opening aligned with the gap.
1 Assignment
0 Petitions

Accused Products

Abstract
In a first aspect, the disclosure features apparatuses for wireless power transfer, the apparatuses including a plurality of magnetic elements joined together to form a magnetic component extending in a plane, where discontinuities in the magnetic component between adjacent magnetic elements define gaps in the magnetic component, a coil including one or more loops of conductive material positioned, at least in part, on a first side of the plane. The apparatuses include a conductive shield positioned on a second side of the plane and which includes one or more openings positioned relative to the gaps.
685 Citations
No References
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20 Claims
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1. An apparatus for wireless power transfer, the apparatus comprising:
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a plurality of adjacent magnetic elements positioned in a plane and defining a gap; a coil comprising one or more loops of conductive material positioned, at least in part, on a first side of the plane and on both sides of the gap; and a conductive shield positioned on a second side of the plane and comprising an opening aligned with the gap. - View Dependent Claims (2, 3, 4, 5, 6, 7)
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8. An apparatus for wireless power transfer, the apparatus comprising:
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a plurality of adjacent magnetic elements positioned in a plane and defining a gap; a coil comprising one or more loops of conductive material positioned, at least in part, on a first side of the plane; and a conductive shield positioned on a second side of the plane and comprising a depression formed in a surface of the shield facing the plane, and aligned with the gap. - View Dependent Claims (9, 10, 11, 12, 13, 14, 15, 16, 17)
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18. An apparatus for wireless power transfer, comprising:
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a plurality of adjacent planar magnetic elements positioned in a plane and defining a gap in the plane; a coil comprising one or more loops of conductive material; and a conductive shield positioned on a second side of the plane and comprising at least one of a depression and an opening formed in a surface of the shield, wherein the at least one of the depression and the opening is aligned with the gap, wherein the coil is oriented so that during operation of the apparatus, the coil generates an average magnetic field oriented in a first direction parallel to the plane. - View Dependent Claims (19, 20)
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1 Specification
This application is a continuation of and claims priority under 35 U.S.C. § 120 to U.S. application Ser. No. 14/688,025, filed on Apr. 16, 2015, which claims priority to U.S. Provisional Patent Application No. 61/980,712, filed on Apr. 17, 2014. The entire contents of the above-referenced applications incorporated herein by reference in their entirety.
This disclosure relates to wireless power transfer.
Energy can be transferred from a power source to a receiving device using a variety of known techniques such as radiative (far-field) techniques. For example, radiative techniques using low-directionality antennas can transfer a small portion of the supplied radiated power, namely, that portion in the direction of, and overlapping with, the receiving device used for pick up. In this example, most of the energy is radiated away in directions other than the direction of the receiving device, and typically the transferred energy is insufficient to power or charge the receiving device. In another example of radiative techniques, directional antennas are used to confine and preferentially direct the radiated energy towards the receiving device. In this case, an uninterruptible line-of-sight and potentially complicated tracking and steering mechanisms are used.
Another approach is to use non-radiative (near-field) techniques. For example, techniques known as traditional induction schemes do not (intentionally) radiate power, but use 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 can transfer modest to large amounts of power over very short distances. In these schemes, the offset tolerances between the power source and the receiving device are very small. Electric transformers and proximity chargers use these traditional induction schemes.
This disclosure relates to wireless transfer systems utilizing wireless power transfer of power from a power transmitting apparatus to a power receiving apparatus. To achieve high power transfer efficiency, the power transmitting apparatus and/or the power receiving apparatus can include a magnetic component and a shield to facilitate the power transfer. Particularly, it can be advantageous to have a large magnetic component in transferring high power for some applications. However, manufacturing the large magnetic component as a single monolithic piece can be impractical or expensive because materials such as ferrites can be difficult to fabricate and/or easily break. Thus, the large magnetic component can instead be formed by combining smaller magnetic elements together. In this approach, the magnetic elements are typically joined across one or more gaps, which can be filled with air or adhesive for connecting the magnetic elements. Such gaps can be problematic, however, because magnetic fields can be concentrated at regions of the gaps. The concentrated magnetic fields can penetrate the nearby shield and other materials or structures and induce eddy currents, thereby leading to losses in the systems and reductions in the amount of power transferred. To address such issues, this disclosure describes a variety of configurations of magnetic components and shields to mitigate losses induced by penetration of magnetic fields into the shields, for example, by aligning openings of the shields to gaps of the magnetic components.
In a first aspect, the disclosure features apparatuses for wireless power transfer, the apparatuses including a plurality of magnetic elements joined together to form a magnetic component extending in a plane, where discontinuities in the magnetic component between adjacent magnetic elements define gaps in the magnetic component, and a coil including one or more loops of conductive material positioned, at least in part, on a first side of the plane. The apparatuses include a conductive shield positioned on a second side of the plane and which the shield includes one or more openings positioned relative to the gaps.
Embodiments of the apparatuses can include any one or more of the following features.
The openings can be respectively aligned with corresponding ones of the gaps. The one or more openings can be positioned relative to the gaps to reduce interactions between magnetic flux crossing the discontinuities and the conductive shield.
The coil can be positioned entirely on the first side of the plane. The one or more loops of conductive material can wrap around the magnetic component. The conductive shield can be substantially parallel to the plane. The one or more openings can extend entirely through the shield.
The plane can extend in orthogonal first and second directions, and where the one or more loops of conducting material wrap around a third direction perpendicular to the first and second directions (i.e., perpendicular to the plane). The gaps can include a first gap having a longest dimension extending in the first direction, and the one or more openings can include a first opening having a longest dimension extending in a direction substantially parallel to the first direction. The first gap can have a maximum width measured in a direction parallel to the second direction, the first opening can have a maximum width measured in a direction parallel to the second direction, and the maximum width of the first opening can be larger than the maximum width of the first gap. A ratio of the maximum width of the first opening to a characteristic size of the magnetic component can be 1:10 or less.
During operation, the coil can generate a magnetic field that oscillates in a direction parallel to the second direction. A first one of the gaps can correspond to a spacing between magnetic elements in a direction parallel to the second direction, and a first one of the one or more openings can be aligned with the first one of the gaps and include a width that extends in a direction parallel to the second direction. Each of the gaps can correspond to a spacing between magnetic elements in a direction parallel to the second direction, and each of the one or more openings can be aligned with a corresponding one of the one or more gaps and includes a width that extends in a direction parallel to the second direction.
The coil can be electrically isolated from the conductive shield.
The one or more loops can include a first plurality of loops concentric about a first axis and a second plurality of loops concentric about a second axis, where the first and second axes are parallel to the third direction. The first plurality of loops can be wound in a first concentric direction about the first axis, and the second plurality of loops can be wound about the second axis in a second concentric direction opposite to the first concentric direction, when measured from an end of the first plurality of loops towards an end of the second plurality of loops. During operation, the coil can generate a magnetic field within the magnetic component that oscillates in a direction parallel to the second direction.
The plurality of magnetic elements can form an array. The plurality of magnetic elements can include 4 or more magnetic elements. At least one of the gaps can include air spaces. At least one of the gaps can include a dielectric material positioned between the magnetic elements. For example, the dielectric material can include an adhesive material.
At least some of the plurality of magnetic elements can be formed of a ferrite material. The ferrite material can include at least one material selected from the group consisting of MnZn-based materials, NiZn-based materials, amorphous cobalt-based alloys, and nanocrystalline alloys.
The coil can be configured to wirelessly transfer power to, or receive power from, another coil. A minimum distance between a surface of the magnetic component and the shield can be 1 mm or less.
At least one of the openings can include lateral surfaces that are angled with respect to the plane.
At least one of the openings can include a triangular cross-sectional profile. At least one of the openings can include a trapezoidal cross-sectional profile. At least one of the openings can include a cross-sectional profile having one or more curved edges.
At least one of the gaps can be with a magnetic material comprising a magnetic permeability different from a magnetic permeability of the plurality of magnetic elements.
In another aspect, the disclosure features apparatuses for wireless power transfer, the apparatuses including a plurality of magnetic elements joined together to form a magnetic component extending in a plane, where discontinuities in the magnetic component between adjacent magnetic elements define gaps in the magnetic component. The apparatuses include a coil comprising one or more loops of conductive material positioned, at least in part, on a first side of the plane, and a conductive shield positioned on a second side of the plane and where the shield includes one or more depressions formed in a surface of the shield facing the magnetic component. Each of the one or more depressions is positioned relative to the gaps.
Embodiments of the apparatuses can include any one or more of the following features.
The one or more depressions can be respectively aligned with corresponding ones of the gaps. The one or more depressions can be positioned relative to the gaps to reduce interactions between magnetic flux crossing the discontinuities and the conductive shield. At least one of the depressions can form an opening that extends entirely through a thickness of the shield.
The coil can be positioned entirely on the first side of the plane. The plane can extend in orthogonal first and second directions, where the one or more loops of conducting material can wrap around a third direction perpendicular to the first and second directions (i.e., perpendicular to the plane). The one or more loops of conductive material wrap around the magnetic component. The conductive shield can be substantially parallel to the plane.
The one or more depressions can include lateral surfaces that are angled with respect to a surface of the shield facing the magnetic component. A width of the one or more depressions measured at the surface of the shield facing the magnetic component can be larger than a width of the one or more depressions measured at another location between the lateral surfaces.
At least one of the depressions can include a cross-sectional profile having a triangular shape. At least one of the depressions can include a cross-sectional profile having a trapezoidal shape. At least one of the depressions can include a cross-sectional profile having one or more curved edges. At least one of the depressions can correspond to a curved groove formed in the shield.
The one or more loops can include a first plurality of loops concentric about a first axis and a second plurality of loops concentric about a second axis parallel to the first axis, and the first and second axes can be orthogonal to the plane of the magnetic component. The first plurality of loops can be wound in a first concentric direction about the first axis, and the second plurality of loops can be wound about the second axis in a second concentric direction opposite to the first concentric direction, when measured from an end of the first plurality of loops towards an end of the second plurality of loops.
During operation, the coil can generate a magnetic field within the magnetic component that oscillates in a direction parallel to a width of at least one of the depressions.
The gaps can include a first gap having a longest dimension extending in a first direction, and the depressions can include a first depression having a longest dimension extending in a direction substantially parallel to the first direction. The first gap can have a maximum width measured in a direction perpendicular to the longest dimension of the first gap. The first depression can have a maximum width measured in a direction perpendicular to the longest dimension of the first depression, and the maximum width of the first opening can be larger than the maximum width of the first gap.
Each of the gaps can correspond to a spacing between magnetic elements in a direction perpendicular to the first direction, and each of the depressions can be aligned with a corresponding one of the gaps and can have a width that extends in a direction perpendicular to the first direction.
The plurality of magnetic elements can form an array. The plurality of magnetic elements can include 4 or more magnetic elements.
At least one of the one or more gaps can include air spaces. At least one of the one or more gaps can include a dielectric material positioned between the magnetic elements. For example, the dielectric material can include an adhesive material.
At least some of the plurality of magnetic elements can be formed of a ferrite material. The ferrite material can include at least one material selected from the group consisting of MnZn-based materials, NiZn-based materials, amorphous cobalt-based alloys, and nanocrystalline alloys.
The coil can be configured to wirelessly transfer power to, or receive power from, another coil.
A ratio of the maximum width of the first depression to a characteristic size of the magnetic component can be 1:10 or less. A minimum distance between a surface of the magnetic component and the shield can be 1 mm or less. At least one of the gaps is filled with magnetic material can have a magnetic permeability different from a magnetic permeability of the magnetic elements.
In another aspect, the disclosure features methods for wirelessly transferring power using apparatuses, the methods including wirelessly transferring power from a power transmitting apparatus to a power receiving apparatus, where at least one of the power transmitting apparatus and the power receiving apparatus includes: a magnetic component extending in a plane and formed from a plurality of magnetic elements joined together, where discontinuities in the magnetic component between adjacent magnetic elements define gaps in the magnetic component, a coil including one or more loops of conductive material positioned, at least in part, on a first side of the plane, and a conductive shield positioned on a second side of the plane and comprising one or more openings positioned relative to the gaps.
The power transmitting apparatus and the power receiving apparatus can each include the magnetic component, the coil, and the conductive shield.
Embodiments of the apparatuses and methods can also include any other features disclosed herein, including features disclosed in connection with other apparatuses and methods, in any combination as appropriate.
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 disclosure, 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.
Like reference numbers and designations in the various drawings indicate like elements.
Introduction
In similar fashion, power receiving apparatus 104 is coupled to a device 108 through a coupling 107. Coupling 107 can be a direct electrical connection or a non-contact inductive coupling. In some embodiments, coupling 107 can include an impedance matching network, as described above.
In general, device 108 receives power from power receiving apparatus 104. Device 108 then uses the power to do useful work. In some embodiments, for example, device 108 is a battery charger that charges depleted batteries (e.g., car batteries). In certain embodiments, device 108 is a lighting device and uses the power to illuminate one or more light sources. In some embodiments, device 108 is an electronic device such as a communication device (e.g., a mobile telephone) or a display. In some embodiments, device 108 is a medical device which can be implanted in a patient.
During operation, power transmitting apparatus 102 is configured to wirelessly transmit power to power receiving apparatus 104. In some embodiments, power transmitting apparatus 102 can include a source coil, which can generate oscillating fields (e.g., electric, magnetic fields) when electrical currents oscillate within the source coil. The generated oscillating fields can couple to power receiving apparatus 104 and provide power to the power receiving apparatus through the coupling. To achieve coupling between power transmitting apparatus 102 and power receiving apparatus 104, the power receiving apparatus 104 can include a receiver coil. The oscillating fields can induce oscillating currents within the receiver coil. In some embodiments, either or both of the source and receiver coils can be resonant. In certain embodiments, either or both of the source and receiver coils can be non-resonant so that the power transfer is achieved through non-resonant coupling.
In certain embodiments, the system 100 can include a power repeating apparatus (not shown in
System 100 can include an electronic controller 103 configured to control the power transfer in the system 100, for example, by directing electrical currents through coils of the system 100. In some embodiments, the electronic controller 103 can tune resonant frequencies of resonators included in the system 100, through coupling 109. The electronic controller 103 can be coupled to one or more elements of the system 100 in various configurations. For example, the electronic controller 103 can be only coupled to power source 106. The electronic controller 103 can be coupled to power source 106 and power transmitting apparatus 102. The electronic controller 103 can be only coupled to power transmitting apparatus 102. In some embodiments, coupling 109 is direct connection. In certain embodiments, coupling 109 is a wireless communication (e.g., radio-frequency, Bluetooth communication). The coupling 109 between the electronic controller 103 can depend on respective one or more elements of the system 100. For example, the electronic controller 103 can be directly connected to power source 106 while wirelessly communicating with power receiving apparatus 104.
In some embodiments, the electronic controller can configure the power source 106 to provide power to the power transmitting apparatus 102. For example, the electronic controller can increase the power output of the power source 106 sent to the power transmitting apparatus 102. The power output can be at an operating frequency, which is used to generate oscillating fields by the power transmitting apparatus 102.
In certain embodiments, the electronic controller 103 can tune a resonant frequency of a resonator in the power transmitting apparatus 102 and/or a resonant frequency of a resonator in the power receiving apparatus 104. By tuning resonant frequencies of resonators relative to the operating frequency of the power output of the power source 106, the efficiency of power transfer from the power source 106 to the device 108 can be controlled. For example, the electronic controller 103 can tune the resonant frequencies to be substantially the same (e.g., within 0.5%, within 1%, within 2%) to the operating frequency to increase the efficiency of power transfer. The electronic controller 103 can tune the resonant frequencies by adjusting capacitance values of respective resonators. To achieve this, for example, the electronic controller 103 can adjust a capacitance of a capacitor connected to a coil in a resonator. The adjustment can be based on the electronic controller 103'"'"'s measurement of the resonant frequency or based on wireless communication signal from the apparatuses 102 and 104. In certain embodiments, the electronic controller 103 can tune the operating frequency to be substantially the same (e.g., within 0.5%, within 1%, within 2%) to the resonant frequencies of the resonators.
In some embodiments, the electronic controller 103 can control an impedance matching network in the system 100 to optimize or de-tune impedance matching conditions in the system 100, and thereby control the efficiency of power transfer. For example, the electronic controller 103 can tune capacitance of capacitors or networks of capacitors included in the impedance matching network connected between power transmitting apparatus 102 and power source 106. The optimum impedance conditions can be calculated internally by the electronic controller 103 or can be received from an external device.
In some embodiments, wireless power transfer system 100 can utilize a source resonator to wirelessly transmit power to a receiver resonator. For example, power transmitting apparatus 102 can include a source resonator that includes a source coil, and power receiving apparatus 104 can include a receiver resonator that includes a receiver coil. Power can be wirelessly transferred between the source resonator and the receiver resonator.
In this disclosure, “wireless energy transfer” from one coil (e.g., resonator coil) to another coil (e.g., another resonator coil) refers to transferring energy to do useful work (e.g., electrical work, mechanical work, etc.) such as powering electronic devices, vehicles, lighting a light bulb or charging batteries. Similarly, “wireless power transfer” from one coil (e.g., resonator coil) to another resonator (e.g., another resonator coil) refers to transferring power to do useful work (e.g., electrical work, mechanical work, etc.) such as powering electronic devices, vehicles, lighting a light bulb or charging batteries. Both wireless energy transfer and wireless power transfer refer to the transfer (or equivalently, the transmission) of energy to provide operating power that would otherwise be provided through a wired connection to a power source, such as a connection to a main voltage source. Accordingly, with the above understanding, the expressions “wireless energy transfer” and “wireless power transfer” are used interchangeably in this disclosure. It is also understood that, “wireless power transfer” and “wireless energy transfer” can be accompanied by the transfer of information; that is, information can be transferred via an electromagnetic signal along with the energy or power to do useful work.
Multiple-Element Magnetic Components
The shield 229 (e.g., a sheet of electrically conductive material) can be positioned adjacent to the source resonator. The shield 229 can be formed of a second conductive material. For example, the shield 229 can be formed from a sheet of material such as copper, silver, gold, iron, steel, nickel and/or aluminum. Typically, the shield 229 acts to shield the resonator from loss-inducing objects (e.g., metallic objects). Further, in some embodiments, the shield 229 can increase coupling of the source resonator to another resonator by guiding magnetic field lines in the vicinity of the source resonator. For example, energy loss from aberrant coupling to loss-inducing objects can be reduced by using the shield 229 to guide magnetic field lines away from the loss-inducing objects.
While
Magnetic components can include magnetic materials. Typical magnetic materials that are used in the magnetic components disclosed herein include materials such as manganese-zinc (MnZn) and nickel-zinc (NiZn) ferrites. MnZn based ferrites can include a MnxZn1-xFe2O4 where x ranges from 0.1-0.9. For example, x can be 0.2-0.8. NiZn based ferrites can include a NixZn1-zFe2O4 ferrite where x ranges from 0.1-0.9. For example, x can be in a range of 0.3-0.4. In some embodiments, magnetic materials can include NiZn based ferrites such as NL12® from Hitachi and 4F1® from Ferroxcube, for example, for operation frequencies of 2.5 MHz or above. In certain embodiments, magnetic materials can include MnZn based ferrites such as ML90S® from Hitachi, for example, for operation frequencies between 500 kHz and 2.5 MHz. In some embodiments, magnetic materials can include MnZn based ferrites such as PC95® from TDK, N95®, N49® from EPCOS and ML24D® from Hitachi, for example, for operation frequencies of 500 kHz or lower. In certain embodiments, magnetic materials can include amorphous cobalt-based alloys and nanocrystalline alloys, for example, for operation frequencies of 100 kHz or lower. Nanocrystalline alloys can be formed on a basis of Fe, Si and B with additions of Nb and Cu. Nanocrystalline magnetic materials can be an alloy of Fe, Cu, Nb, Si and B (e.g., Fe73.5Cu1Nb3Si15.5B7). In some embodiments, nanocrystalline magnetic materials can be an alloy of Fe, Co, Zr, B and Cu. In certain embodiments, nanocrystalline magnetic materials can be an alloy of Fe, Si, B, Cu and Nb. In certain embodiments, nanocrystalline magnetic materials can be an alloy of Fe, Co, Cu, Nb, Si and B. The nanocrystalline magnetic materials can include an alloy based on Fe. For example, the alloy can be a FeSiB alloy.
While these materials are generally available in small sizes, some applications for wireless power transfer utilize magnetic components with a large areal size. For example, a car battery charging application may need to use a large areal size (e.g., 30 cm×30 cm) magnetic component to transfer high power of 1 kW or more (e.g., 2 kW or more, 3 kW or more, 5 kW or more, 6 kW or more).
In some embodiments, a single monolithic piece of magnetic components can be utiltized when the single monolithic piece of the required size is available. In some embodiments, it can be difficult and/or expensive to manufacture a monolithic piece of magnetic component such as MnZn or NiZn ferrites with a large areal size (e.g., 30 cm×30 cm) needed for the high power transfer. Moreover, MnZn and NiZn ferrites can be brittle, and accordingly, large-area pieces of these materials can be highly susceptible to breakage. To overcome such difficulties when fabricating the magnetic components disclosed herein, ferrite materials can be manufactured in pieces of small areal size (e.g., 5 cm×5 cm), and several such pieces can be joined together to form a larger combined magnetic component. These smaller magnetic elements can behave functionally in a very similar manner as a larger magnetic element when they are joined.
However, joining multiple smaller magnetic elements to form a larger magnetic component can introduce gaps and certain inhomogeneities relative to a single sheet of magnetic component. In particular, irregularities at the edges of the small pieces can lead to “magnetic field hot spots,” where magnetic fields are locally concentrated at the irregularities. Magnetic field hot spots due to irregularities at the edges of the joined pieces of magnetic component can damage the magnetic component due to heating, and/or reduce the quality factor of the apparatus.
In some embodiments, a gap can be formed between two pieces of magnetic elements. The gap can be an air gap, or can be filled with a dielectric material such as adhesive or a type of material different from the material of the magnetic elements (e.g., ferrite). When magnetic fields oscillate substantially perpendicular to interfaces of the gap, the magnetic fields can be concentrated with high density within the gap. In addition, magnetic fields can also be concentrated with high density at locations above or below the gap, and these concentrated magnetic fields can penetrate a portion of a shield at positions above or below or in the general vicinity of the gap. Such penetration can lead to loss of energy by generating eddy currents and heat in the corresponding portions of the shield. Similarly, strongly localized magnetic field hot spots induced by irregularities in the magnetic component may penetrate the shield and lead to loss of energy. To illustrate this phenomena,
To mitigate such energy losses, this disclosure features shield geometries that reduce the effects of hot spots and concentrated magnetic fields due to irregularities at the edges and gaps of joined magnetic elements (e.g., pieces of magnetic component). In particular, energy losses due to the penetration of magnetic fields into shield 229 can be reduced by forming openings in the shield 229 and/or by modifying the shape of shield 229 in regions where the magnetic field density is locally increased, e.g., in regions corresponding to gaps between the magnetic elements. By adjusting the shape of the shield 229, the extent to which the magnetic field 304 penetrates the shield 229 can be reduced, thereby mitigating energy losses.
The shields disclosed herein allow the use of magnetic components of large areal sizes (e.g., by joining many smaller pieces of magnetic component) while reducing energy losses due to interactions between the shield and concentrated magnetic fields. As a result, apparatuses that include the shields disclosed herein can achieve high power transfer efficiencies and can operate over a wide range of power transfer levels (e.g., between 0.5 kW to 50 kW). For example, the power transfer can be 3.3 kW or more (e.g., 6.6. kW or more).
Shield Configurations
In
The shield 230 lies in a plane nominally parallel to another plane in which the coil 210 lies. In this example, the magnetic component 220 lies in a plane parallel to another plane in which the coil 210 lies. In certain embodiments, the magnetic component 220 lies in a plane substantially parallel (e.g., within 3°, within 5°, within 10°, within 15°) to another plane in which the coil 210 lies.
The magnetic component 220 includes four magnetic elements 410, 412, 414 and 416 (e.g., ferrite tiles) each shaped as a rectangular slab. The magnetic elements are joined together with a dielectric material 420 to form the magnetic component 220, which extends in a plane parallel to the A-B plane. In this example, the dielectric material 420 is an adhesive material which bonds the four magnetic elements 410, 412, 414 and 416 together. As explained previously, by fabricating a magnetic component from smaller magnetic elements, large-size magnetic components can be produced more easily and at lower cost compared to fabrication methods that rely on producing monolithic elements. By using multiple small magnetic elements to form a larger magnetic component, the size of the magnetic component can generally be selected as desired for a particular apparatus. In some embodiments, the size of the magnetic component can have an area of 30 cm×30 cm or larger (e.g., 40 cm×40 cm or larger, 50 cm×50 cm or larger).
In some embodiments, the magnetic component 220 can be formed from a plurality of tiles, blocks, or pieces of magnetic component that are arranged together to form magnetic component 220. The plurality of tiles, blocks, or pieces can all be formed from the same type of magnetic component, or can be formed from two or more different types of magnetic components. For example, in some embodiments, materials with different magnetic permeability can be located at different positions of the magnetic component 220. A dielectric material such as adhesive can be used to glue the different magnetic elements together. In some embodiments, magnetic elements can be in direct contact with one another. Irregularities in interfaces between the direct contact can lead to magnetic field hot spots. In some embodiments, the magnetic component 220 can include electrical insulator layers, coatings, strips, adhesives for mitigating build-up of heat at irregular interfaces within the magnetic component 220.
Referring back to
The coil 210 has a plurality of loops which lie in the A-B plane, and includes windings 451 and 452. The windings 451 and 552 correspond to first and second plurality of loops, respectively of the coil 210. The winding 451 has an end 401 and connects to the winding 452, which has an end 403. In this example, starting from the end 401, the winding 451 is concentrically wound around an axis 402 (starting from the inner winding of winding 452 towards its outer winding), which points into the drawing plane in (i.e., negative C-direction in
The coil 210 is configured to generate oscillating magnetic fields and magnetic dipoles in the magnetic component 220, which oscillate substantially along the B-axis, when currents oscillate within the coil 210. The plurality of loops of the coil 210 define a coil that is positioned in the A-B plane. More generally, the coil 210 may form a flat portion of the coil 210 that is oriented at an angle to the A-B plane. For example, the angle can be within 5° or less (e.g., 10° or less, 15° or less, 20° or less). Generally, either or both of the axes 402 and 404 may point at an angle with respect to the C-direction. For example, the angle can be within 5° or less (e.g., 10° or less, 15° or less, 20° or less). In this disclosure, the “x” notation (e.g., of axis 402) refers to a direction pointing into the drawing plane (i.e., negative C-direction in
In this disclosure an “average magnetic field” of a magnetic component at a given time refers to the magnetic field integrated over the total volume of all magnetic elements in the magnetic component at the given time. Referring back to
The oscillating electrical current in the coil 210 generates magnetic fields within the magnetic component 220. To illustrate this, the power transmitting apparatus 102 shown in
Generally, when the coil 210 generates magnetic fields in the magnetic component 220 with the average magnetic field 471 pointing along the direction 441 at a given time, high densities of magnetic fields become concentrated in the gap 422. Moreover, irregularities at interfaces 432 and 434 of the gap 422 can contribute to form magnetic field hot spots.
In some embodiments, strongly localized magnetic field hot spots can be formed within the gap 422. For example, as shown in
For example, magnetic fields 520 depicted as dashed arrows within region 510 concentrate on the peak 512. Concentrated field regions (e.g., region 510) may lead to increased heating, material breakdown, and/or damaging of the magnetic component, which can lead to deteriorated power transfer efficiency provided by the power transmitting apparatus 102.
Magnetic field hot spots can become more pronounced when the distance between the interfaces 432 and 434 is decreased. The distance between the interfaces 432 and 434 can be reduced (for example, when elements 410 and 416 are joined together more closely) to achieve a more compact arrangement of the magnetic elements 410 and 416. Polishing the interfaces can, in certain embodiments, assist in reducing the extent of irregularities at the surfaces. However, it has generally been found that mechanical polishing alone does not fully ameliorate surface irregularities that lead to magnetic hot spots.
In the examples shown in
For a conventional shield without opening 560, the magnetic fields 525 below the gap 422 would penetrate the shield. Because the magnetic fields 525 can be strong due to the gap as described above, such penetration can induce large eddy currents which can generate heat in the shield. This leads to energy losses in the power transmitting apparatus 102. If the conventional shield were moved closer to the gap 422, the losses become even larger as magnetic fields 525 induce stronger eddy currents in the shield.
However, unlike conventional shields, the shield 230 has its opening 560 aligned to the gap between magnetic elements 410 and 416 and located in a region of the magnetic fields 525. As a result, the penetration of fields 525 into shield 230 is significantly reduced or even eliminated, thereby mitigating the generation of strong eddy currents in the shield 230. Thus, energy losses due to the shield 230 can be reduced or even eliminated, relative to energy losses that would otherwise occur due to a conventional shield.
Electromagnetic simulations can be used to predict and to compare characteristics of various power transmitting apparatuses.
Typically, wireless power transfer using high Q-factor resonators can be efficient because the high Q-factor can lead to large energy transfer efficiency between resonators. Furthermore, quality factor Qtrans of an apparatus and quality factor contributed by a shield Qshield (which will be described in greater detail in a later section) can be indicators of how efficient the power transfer can be between apparatuses. In the following, the quality factor Qtrans of an apparatus and the quality factor contributed by a shield to an apparatus, Qshield, are discussed. A smaller value of quality factor Qtrans can lead to smaller energy transfer efficiency between apparatuses.
Electromagnetic simulations can be used to compare characteristics of systems with different distances between magnetic component and shields. Generally, the minimum distance between any point on the surface of magnetic component 220 and any point on the surface of shield 229 can be 1 mm or less (e.g., 2 mm or less, 5 mm or less, 10 mm or less, 15 mm or less, 20 mm or less).
As previously described, energy loss due to penetration of magnetic fields into shield 229 can be reduced by forming openings in the shield 229 where the magnetic field density is locally increased, e.g., in regions corresponding to gaps between the magnetic elements.
In the example shown in
When coil 210 generates a magnetic field within gap 422 of the magnetic component 220 in a direction parallel to the B-direction, a portion of the magnetic field 525 extends below gap 422 and penetrates shield 229, which leads to energy loss, as discussed previously. The penetration of portion 525 of the magnetic field into shield 229 is shown on
In apparatus 1000, however, penetration of magnetic field 525 into shield 230 is reduced or eliminated because opening 560 is aligned with gap 422, and therefore positioned at the location where magnetic field 525 extends below gap 422. Because there is no shield material where magnetic field 525 extends below the gap 422, the effect of magnetic field 525 on shield 230 is significantly mitigated relative to apparatus 720.
In general, the opening 560 can be located where the magnetic field below the magnetic component 420 is particularly strong due to fringe effects or hot spots. By providing an opening in a region of the shield where strong magnetic fields would otherwise penetrate the shield, energy losses due to the shield can be reduced or eliminated. Accordingly, one or more openings of the shield 230 can be respectively aligned with corresponding ones of the one or more gaps of the magnetic component 220. The relative positioning of the one or more openings with respect to the one or more gaps can reduce interactions between magnetic flux of the magnetic fields crossing discontinuities of the magnetic component 220 and the shield 230. Moreover, the absence of shield material can lead to a lighter weight shield and reduce shield material costs.
In
The width 1009 of opening 560 of shield 230 can be selected to provide reduced energy loss due to magnetic field penetration into the shield 230, while at the same time shield 230 still effectively shields magnetic fields from lossy objects.
Generally, an opening 560 can have a width 1009 in a direction parallel to oscillations of magnetic fields within a gap of a magnetic component 220. Referring back to
In certain embodiments, a ratio of the width 1009 to width 424 can be 10:5 or less (e.g., 10:2.5 or less, 10:2 or less, 10:1 or less, 10:0.5 or less, 10:0.4 or less, 10:0.2 or less). A high ratio may lead to a higher Qshield. In some cases, if the ratio of the width 1009 to width 424 is too large, the shield 230 may not effectively shield lossy objects. In some embodiments, the ratio of the width 1009 to width 424 is not larger than 100:1 (e.g., not larger than 50:1, not larger than 25:1). For example, the ratio of the width 1009 to width 424 can be about 100:1 rather than 25:1 when the width 424 is smaller compared to the case when it is larger.
In some embodiments, gap 422 can have a minimum width of 0.2 mm or more (e.g., 0.5 mm or more, 1 mm or more, 1.5 mm or more, 2 mm or more). Opening 560 can have a minimum width of 1 mm or more (e.g., 2 mm or more, 4 mm or more, 8 mm or more, 10 mm or more, 15 mm or more).
In some embodiments, width 1009 of opening 560 can be equal to or less than width 424 of gap 422. Such a configuration may be utilized, for example, when a thickness of shield 230 is about a skin depth or less (e.g., half the skin depth) of the shield material and/or one or more lossy objects are close by (e.g., within 3 mm) to the shield 230. The skin depth of the shield material is the length of material through which the oscillating magnetic fields at the operating frequency pass before their amplitudes have decayed by a factor 1/e. In this case, if the width 1009 is larger than the width 424, concentrated magnetic fields within gap 422 can still interact with the lossy object because the thickness of shield 230 is relatively thin and/or the lossy object is close to the shield 230. Therefore, in this case, it can be desirable to have width 1009 to be equal or less than width 424 although magnetic fields may still penetrate the shield 230.
In this disclosure, a characteristic size of the magnetic component 220 is defined as the radius 1011 of the smallest sphere that fits around the magnetic component 220 as illustrated in
Referring to
Referring back to
As described above, in some embodiments, the width of opening 560 can be selected based on the width of gap 422. To choose the width of opening 560, a plot such as plot 1400 can be used. In certain embodiments, where width of gap 422 is fixed, the width of opening 560 can be selected. For example, for a width of 0.2 mm of gap 422, the width of opening 560 can be selected to be 4 mm over 10 mm. For a width of 1.8 mm of gap 422, the width of opening 560 can be selected to be 10 mm over 4 mm according to plot 1400. Other widths than 4 mm and 10 mm of opening 560 can be selected to have a higher Qshield depending on a fixed width of gap 422.
Openings in the shield can generally be implemented in a variety of ways. In some embodiments, a shield can be segmented into two pieces like the example shown in
The strength of the magnetic field 525 typically decays away from the surface of magnetic component 220 according to a power law of the ratio (α) of the width of gap 422 (i.e., width 424 in
More generally, a magnetic component can be formed in a way that multiple gaps exist and magnetic fields oscillate perpendicular to surfaces of the gap, for example, as described above. In this case, multiple openings and notches can be formed in the shield to reduce power dissipation and energy loss due to the shield positioned below the magnetic component. The openings and notches can form depressions in the shield that extend only partially through a thickness of the shield, or can extend completely through the shield. In similar manner described in preceding paragraphs, the depressions can be positioned to be respectively aligned with corresponding gaps of the magnetic component. The depressions can be positioned relative to the gaps to reduce interactions between magnetic flux of magnetic fields crossing discontinuities of the magnetic component and the shield.
In the example shown in
In some embodiments, openings formed in the shield have lateral surfaces that are orthogonal to the surface of the shield that faces the magnetic component. More generally, however, openings formed in the shield can have lateral surfaces with a variety of orientations with respect to the surface of the shield that faces the magnetic component.
During use of a power transmitting apparatus, magnetic component 220 can become damaged, which may lead to the formation of hot spots. The existence and/or development of hot spots can be monitored using a thermal detector with appropriate spatial resolution. For example, the thermal detector can measure localized high temperature points which can correspond to damage or defects in the magnetic component 220. Then openings or notches described in detail above can be formed into a shield based on the monitored hot spots to accommodate the presence of hot spots.
In some embodiments, the width of gap 422 between elements of the magnetic component can vary, and accordingly, an opening of shield 230 can have a varying width to match the varying width of gap 422. To illustrate this,
The varying width of the gap leads to varying magnetic resistance of the magnetic component 220 along the A-direction. Accordingly, when the coil 210 generates magnetic field within the magnetic component 220, magnetic elements 1910 can be arranged so that the varying magnetic resistance provides a more uniform distribution of magnetic fields than would otherwise be possible with a gap of constant width in the B-direction, thereby leading to less power dissipation in the magnetic component 220.
For magnetic components with gaps between elements that vary in width, opening 1921 of the shield 1920 can also have varying width to match the varying width of the gap between magnetic elements 1910 to mitigate concentration of penetration of magnetic fields into the shield 1920.
In some embodiments, a dielectric material or magnetic material can fill in gap 422 of a magnetic component 220. The dielectric material (e.g., coolant liquids) or magnetic material filling the gap 422 can have high thermal conductivity and be placed between magnetic elements to facilitate the dissipation of heat generated within the magnetic elements. Referring to
In the example shown in
In some embodiments, magnetic elements can be joined together by an adhesive tape. For example,
In addition to the shield geometries disclosed above for mitigating energy losses due to penetration of the magnetic fields from the magnetic component into the shield, other techniques can also be used to reduce energy losses.
In some embodiments, for example, energy losses due to penetrating magnetic fields can be reduced by adjusting the magnetic field distribution within the magnetic component.
The magnitudes and phases of the applied currents in each of the two coils 2040 and 2041 can be selected to control a uniformity of magnetic field distribution induced in the magnetic component 220. A more uniform distribution can lead to less hot spots and energy losses of the magnetic fields within the magnetic component 220. In contrast, less uniform magnetic distribution may localize fields into hot spots. The magnitudes and phases can be selected depending on the geometry and/or properties of the magnetic component 220.
Non-uniform magnetic field distributions within the magnetic component lead to the formation of hot spots, because power is dissipated locally in proportion to the square of the magnetic field amplitude. Moreover, a non-uniform magnetic field distribution increases the loss coefficient of the magnetic component. Both of these effects lead to a reduced quality factor for a resonator that includes the magnetic component, and can even cause the magnetic component to saturate at lower power levels.
However, these effects can be mitigated by generating a more uniform magnetic field distribution within the magnetic component, as described above. In particular, because power dissipation varies approximately proportionally to the square of the magnetic field amplitude, for a fixed total magnetic flux through a magnetic component, a configuration with a more uniform field distribution will generally exhibit lower losses than a configuration with a more non-uniform field distribution. The effect is analogous to the electrical resistance of an electrical conductor, where decreasing the effective cross-sectional area of the conductor leads to higher resistance, for example, due to the skin effect.
In some embodiments, magnetic elements positioned below coil 2040 can have a different magnetic resistance than the magnetic elements positioned below coil 2041 due to manufacturing imperfections that lead to different sizes of magnetic elements and/or different magnetic permeabilites of the magnetic elements. For example, magnetic elements positioned below coil 2040 can have a magnetic permeability smaller by 2% or more (e.g., 5% or more, 10% or more) than that of magnetic elements positioned below coil 2041 due to fabrication tolerances and/or errors.
To circumvent such imperfections, coil 2040 can operate with current having a magnitude that is larger by 2% or more (e.g., 5% or more, 10% or more) than that of coil 2041. The phase difference of currents between the coils 2040 and 2041 can be 10° or more (e.g., 20° or more, 30° or more) to match a magnitude of the currents at a given time. Such approaches may lead to a more uniform magnetic field distribution, thereby reducing the formation of hot spots that lead to magnetic fields bending outwards from gaps between the elements of magnetic component 220, and also reducing energy losses of the magnetic fields within the magnetic component 220. In some embodiments, either or both of two coils 2040 and 2041 can have varying diameters of wire in a similar manner described in relation to coil 210 in
By providing a coil with an increased spacing 2111 (e.g., relative to spacing 2112) between adjacent loops in the region of coil 210 that is near gap 422 (not shown) in the magnetic component, the concentration of magnetic fields within gap 422 can be reduced, because less dense coil windings can induce weaker magnetic fields. Thus, penetration of magnetic fields into an adjacent shield can be reduced. Moreover, variations in spacings between adjacent wire portions in coil 210 can be used to control a uniformity of magnetic field distribution induced in magnetic component 220, leading to less hot spots and energy losses of the magnetic fields.
The coil 2204 is wound around the magnetic component 220, which can have one or more gaps 422 (not shown) as described above. The gaps may lead to concentrated magnetic fields penetrating into the shield 2206. Accordingly, the shield 2206 can have an opening 2210 aligned to a gap 422 of the magnetic component 220 to mitigate the magnetic field penetration.
The apparatus 2300 can include a shield 2320 positioned adjacent to the magneti