Method and apparatus for the measurement of radio-frequency electric permittivity by a meander-line ring resonator

• US 9,151,787 B2
• Filed: 11/01/2012
• Issued: 10/06/2015
• Est. Priority Date: 01/13/2012
• Status: Active Grant

• Current Assignee: United States Secretary of the Army
• Original Assignee: The United States Of America As Represented By The Secretary Of The Army
• Inventors: Mazzaro, Gregory J.
• Primary Examiner(s): TANG, MINH NHUT
• Application Number:
  US13/666,404
• Publication Number:
  US 20130181725A1
• Time in Patent Office: 1,069 Days
• US Class Current: 1/1
• CPC Class Codes: G01R 27/04 in circuits having distributed constants , e.g. having very long conductors or involving high frequencies
• CPC Class Codes: G01R 27/2623 Measuring-systems or electronic circuits G01R27/2635, G01R27/2682 take precedence
• CPC Class Codes: H01P 7/00 Resonators of the waveguide type
• CPC Class Codes: H01P 7/082 Microstripline resonators H01P7/088 takes precedence

Abstract

Methods and apparatus for measuring permittivity having a meander-line ring resonator, which may be disposed on a substrate proximate to and separated from an input coupler and an output coupler thereon, the resonator ring further including a continuous conductive material having at least two turns to form a single congruent pattern, symmetrical along at least one axis.

Claims

1. An apparatus for measuring permittivity comprising:

a meander-line ring resonator, proximate to and separated from an input coupler and an output coupler, the meander-line ring resonator comprising a resonating ring formed of a continuous conductive material having at least two turns to form a single congruent pattern, symmetrical along at least one axis of the resonating ring and completely enclosing an area therewithin; and

a microcontroller configured to measure permittivity of a sample positioned in the vicinity of the meander-line ring resonator based on a frequency shift in the electric field of the meander-line resonator caused by the sample.

2. The apparatus of claim 1, further comprising:

the input coupler positioned on a side of the meander-line ring resonator, the input coupler elongated to conform to the side of the meander-line ring resonator; and

the output coupler positioned on an opposite side of the meander-line ring resonator, the output coupler elongated to conform to the opposite side of the meander-line ring resonator.

3. The apparatus of claim 2, wherein the input coupler and output coupler are comprised of a curved length that is a substantial percentage of the meander-line ring resonator.

4. The apparatus of claim 1, wherein the at least two turns further comprise at least one pair of arcuate portions and at least one pair of serpentine portions.

5. The apparatus of claim 4, wherein the input coupler and output coupler are arcuate and are substantially parallel, spaced apart from the arcuate portions of the meander-line ring resonator.

6. The apparatus of claim 4, wherein the at least one pair of serpentine portions further comprise at least three continuous symmetrical turns along the at least one axis.

7. The apparatus of claim 1, wherein the resonator is configured to resonate at a frequency below 1 GHz.

8. The apparatus of claim 1, wherein the at least one axis is coincident with input and output lines of the input and output couplers.

9. The method of assembling the apparatus of claim 1 comprising:

providing a ground plane; and

positioning the meander-line ring resonator on a different plane than the ground plane so as to improve permittivity measurement.

10. A method of modifying the apparatus of claim 1 comprising:

reducing the separation between the input and output couplers and the meander-line ring resonator and/or widening the length of the input and output couplers proximate to the meander-line ring resonator so as to decrease transmission loss of the meander-line ring resonator.

11. A method of modifying the apparatus of claim 1 comprising:

increasing the number of turns of the resonating ring while maintaining the same initial path length of the resonating ring so as to reduce the area enclosed by the resonating ring.

12. A method of using the apparatus of claim 1 comprising:

positioning the meander-line ring resonator in the vicinity of a sample;

measuring a frequency shift in the electric field of the meander-line resonator caused by the sample; and

determining the permittivity of the sample based on the measured frequency shift.

13. The apparatus of claim 1, wherein meander-line ring resonator comprises six, eight or twelve turns.

14. A method for measuring permittivity of a sample based on a change in the electric field comprising:

capacitively coupling a radio-frequency (RF) signal from an input coupler across a first gap to a meander-line ring resonator, where the meander-line ring resonator comprises a resonating ring formed of continuous conductive material on a substrate with at least two turns to form a single congruent pattern symmetrical along at least one axis of the resonating ring and completely enclosing an area therewithin;

resonating the RF signal within the meander-line ring resonator;

capacitively coupling the RF signal to the output coupler across a second gap to the meander-line ring resonator;

positioning the meander-line ring resonator in the vicinity of a sample; and

measuring permittivity of the sample based on a frequency shift in the electric field of the meander-line resonator caused by the sample.

15. The method of claim 14, further comprising:

receiving the RF signal using an input line connected to the input coupler on a side of the meander-line ring resonator, the input coupler being elongated to conform to the side of the meander-line ring resonator; and

outputting the RF signal using an output line connected to the output coupler on an opposite side of the meander-line ring resonator, the output coupler being elongated to conform to the opposite side of the meander-line ring resonator.

16. The method of claim 14, wherein the turns comprise at least one pair of arcuate portions and at least one pair of serpentine portions.

17. The method of claim 14, wherein the input coupler and output coupler are comprised of a curved length that is a substantial percentage of the meander-line ring resonator.

18. The method of claim 14, wherein the meander-line ring resonator further comprises at least three continuous symmetrical turns along the at least one axis.

19. The method of claim 14, wherein the meander-line ring resonator resonates at a frequency below 1 GHz.

20. The method of claim 14, further comprising:

storing the signal in memory; and

subsequently positioning a dielectric sample proximate the meander-line ring resonator to generate a change in the frequency response of the meander-line ring resonator.

21. The method of claim 20, further comprising:

comparing the frequency response change with the previously stored data signal of the meander-line ring resonator when no dielectric sample was applied to determine permittivity.

22. A system for providing a portable permittivity measurement of a sample comprising:

a substrate;

an input coupler and an output coupler;

the input coupler positioned separate from and opposite to an output coupler on the substrate;

a meander-line ring resonator, proximate to and separated from the input coupler and the output coupler, the meander-line ring resonator comprising a resonating ring formed of a continuous conductive material having at least two turns to form a single congruent pattern, symmetrical along at least one axis of the resonating ring and completely enclosing an area therewithin; and

a portable computer coupled to the meander-line ring resonator, wherein the portable computer is configured to send a radio-frequency (RF) signal to the input coupler and to receive a RF signal from the output coupler and to measure permittivity of a sample positioned proximate the meander-line ring resonator, wherein the sample causes a change in the frequency response of the meander-line ring resonator.

23. The system of claim 22, further comprising:

memory configured to store the signal.

24. The system of claim 23, further comprising:

a microprocessor configured to compare the frequency response change with the previously stored signal of the meander-line ring resonator when no dielectric sample was applied to determine permittivity.