Imaging and Sensing of Thin Layer Using High-Frequency Ultrasonic Transducers
US-2024036005-A1 · Feb 1, 2024 · US
US10697827B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10697827-B2 |
| Application number | US-201414528847-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 30, 2014 |
| Priority date | Jun 16, 2014 |
| Publication date | Jun 30, 2020 |
| Grant date | Jun 30, 2020 |
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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.
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We claim: 1. A method comprising: receiving an electrical measurement signal from a sensor having a protective screen, wherein the measurement signal includes distortion due to a resonant frequency of the sensor; applying, to the measurement signal, an analog complementary compensation filter circuit adapted to compensate for distortion in the measurement signal caused by the protective screen, the complementary compensation filter comprising a second order transfer function to the measurement signal to produce a compensated frequency response signal, wherein applying the complementary compensation filter circuit reduces the distortion to less than 1 dB for frequencies ranging from zero to 60% 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 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. 4. The method of claim 3 , further comprising: determining a frequency response complementary to the frequency response of the sensor. 5. The method of claim 3 , further comprising: determining a quality factor associated with a frequency response of the sensor. 6. The method of claim 5 , further comprising: determining parameters of the compensation filter circuit corresponding to a frequency response and quality factor complementary to the frequency response of the sensor. 7. 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 the frequency variable, f n is the resonant frequency of the transducer, and Q is a quality factor associated with the sensor frequency response. 8. 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 transducer, and Q is a quality factor associated with the sensor frequency response. 9. The method of claim 1 , wherein the sensor comprises a diaphragm having a resonant frequency modeled by f = 36 2 π E t 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, v is Poisson's ratio of the diaphragm material,
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