IP Library Granted Patent US 11,255,718
Granted Patent B2
US 11,255,718 · App. 15/929,574 · Granted Feb 22, 2022

Systems and methods for extending frequency response of resonant transducers

Inventors: Joe VanDeWeert (Maywood, NJ); Adam Hurst (New York, NJ); Joseph Carter (League City, TX); Douglas R. Firth (Ithaca, NY); Alan R. Szary (Ithaca, NY)
Assignee: Kulite Semiconductor Products, Inc.
G01H13/00G01H11/08G01L9/065G01L9/0047
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Quick Facts
Patent No.
US 11,255,718
App. No.
15/929,574
Granted
Feb 22, 2022
Kind
B2
Abstract

Certain implementations of the disclosed technology may include systems and methods for extending a frequency response of a transducer. A method is provided that can include receiving a measurement signal from a transducer, wherein the measurement signal includes distortion due to a resonant frequency of the transducer. The method includes applying a complementary filter to the measurement signal to produce a compensated signal, wherein applying the complementary filter reduces the distortion to less than about +/−1 dB for frequencies ranging from about zero to about 60% or greater of the resonant frequency. The method further includes outputting the compensated signal.

Claims (211)

1. A method comprising:

receiving, responsive to an applied pressure, an electrical measurement signal from a sensor having a protective screen, wherein the measurement signal includes a distortion due to the protective screen;

applying, to the measurement signal, a complementary compensation filter circuit adapted to compensate for the distortion in the measurement signal, wherein applying the complementary compensation filter circuit reduces the distortion to less than 1 dB for frequencies ranging from zero up to 60% of a resonant frequency and less than 2 dB for frequencies ranging from over 60% to 90% of the resonant frequency; and

outputting the compensated signal, wherein the compensated signal reduces a resonance associated with the sensor.

2. The method of claim 1 , wherein applying the complementary compensation filter circuit to the measurement signal comprises applying a second order transfer function to the measurement signal to produce a compensated frequency response signal filter having a frequency response based on an inverse frequency response of the sensor, wherein the second order transfer function is implemented by a double integrator with feedback.

3. The method of claim 1 , further comprising;

determining the resonant frequency associated with a frequency response of the sensor; and

determining a quality factor complementary to the frequency response of the sensor.

4. The method of claim 3 , further comprising:

determining a compensated frequency response of the sensor based on one or more of the determined resonant frequency and the determined quality factor.

5. The method of claim 1 , wherein the complementary compensation filter circuit is an analog circuit.

6. The method of claim 1 , wherein the complementary compensation filter circuit includes a Helmholtz frequency response, T c (f), represented by the equation:

T

C

(

f

)

=

-

f

2

+

i

f

f

n

Q

+

f

n

2

-

f

2

+

i

f

f

n

+

f

n

2

wherein f is a frequency variable, f n is the resonant frequency of the sensor, and Q is a quality factor associated with the sensor frequency response.

7. The method of claim 1 , wherein the complementary compensation filter circuit includes a seismic mass frequency response, T c (f), represented by the equation:

T

C

(

f

)

=

-

f

2

+

i

f

f

n

Q

+

f

n

2

f

n

2

wherein f is the frequency variable, f n is the resonant frequency of the sensor, and Q is a quality factor associated with the sensor frequency response.

8. The method of claim 1 , wherein the sensor comprises a diaphragm having a resonant frequency modeled by

f

=

3

6

2

π

Et

2

12

ρ

a

4

(

1

-

v

2

)

and wherein the diaphragm is flat and square having a length a and thickness t, and where E is Young's modulus, ν is Poisson's ratio of the diaphragm material, and ρ is the applied pressure measured in Pascals.

9. The method of claim 1 , wherein the distortion is further due to a resonance of the sensor.

10. A filter comprising:

a measurement input terminal adapted to receive an electrical measurement signal from a sensor having a protective screen responsive to a pressure applied to a diaphragm of the sensor, wherein the measurement signal includes a distortion due to the protective screen associated with the sensor;

a complementary filter compensation circuit adapted to compensate for the distortion in the measurement signal, the complementary filter compensation circuit adapted to receive and compensate a frequency response of the measurement signal and to reduce the distortion to less than 1 dB for frequencies ranging from zero up to 60% of a resonant frequency and less than 2 dB for frequencies ranging from over 60% to 90% of the resonant frequency; and

an output terminal for outputting the compensated signal, wherein the compensated signal reduces a resonance associated with the sensor.

11. The filter of claim 10 , wherein the compensation circuit comprises second order transfer function implemented by a double integrator with feedback.

12. The filter of claim 10 , wherein a response of the compensation circuit is configured based on one or more of the resonant frequency and a quality factor associated with the sensor.

13. The filter of claim 10 , wherein the compensation circuit comprises a Helmholtz frequency response, T c (f), represented by the equation:

T

C

(

f

)

=

-

f

2

+

i

f

f

n

Q

+

f

n

2

-

f

2

+

i

f

f

n

+

f

n

2

wherein f is the frequency variable, f n is the resonant frequency of the sensor, and Q is a quality factor associated with a frequency response of the sensor.

14. The filter of claim 10 , wherein the compensation circuit comprises a seismic mass frequency response, T c (f), represented by the equation:

T

C

(

f

)

=

-

f

2

+

i

f

f

n

Q

+

f

n

2

f

n

2

wherein f is the frequency variable, f n is the resonant frequency of the sensor, and Q is a quality factor associated with a frequency response of the sensor.

15. The filter of claim 10 , further comprising a sensor, wherein the sensor comprises a diaphragm having a resonant frequency modeled by

f

=

3

6

2

π

Et

2

12

ρ

a

4

(

1

-

v

2

)

wherein the diaphragm is flat and square having a length a and thickness t, and where E is Young's modulus, ν is Poisson's ratio of the diaphragm, and ρ is an applied pressure measured in Pascals.

16. The filter of claim 10 , wherein the compensation circuit comprises a low-pass filter configured to attenuate measurement signal frequencies or compensated signal frequencies above the resonant frequency.

17. The filter of claim 16 , wherein the low-pass filter comprises a 6-pole filter having a 48 dB/octave roll-off.

18. The filter of claim 10 , further comprising a sensor, wherein the sensor comprises an accelerometer.

19. The filter of claim 18 , wherein the sensor includes one or more piezoresistive elements in communication with a diaphragm.

20. The filter of claim 10 , wherein the compensation circuit is an analog circuit comprising one or more of an amplifier, a summing block, an integrator, and a band-pass filter.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 13, 2020
From: HURST, ADAM; VANDEWEERT, JOSEPH R.; CARTER, JOSEPH; FIRTH, DOUGLAS R.; SZARY, ALAN R.
To: KULITE SEMICONDUCTOR PRODUCTS, INC.
Reel/Frame 052648/0541 →
Continuity (3)
Continuation 14528847 · Oct 30, 2014
Provisional Application 62012764 · Jun 16, 2014
Related Publication 20200271510A1 · Aug 27, 2020