Electronically tunable resonant accelerometer

• US 4,197,478 A
• Filed: 01/25/1979
• Issued: 04/08/1980
• Est. Priority Date: 01/25/1979
• Status: Expired due to Term

• Current Assignee: Southwest Research Institute
• Original Assignee: Southwest Research Institute
• Inventors: Silvus, Howard S. Jr.
• Primary Examiner(s): Budd, Mark O.
• Application Number:
  US06/006,285
• Time in Patent Office: 439 Days
• Field of Search: 310/314, 310/316, 310/317, 310/329, 310/321, 310/325, 310/326, 310/328, 310/332, 310/331, 340/10, 73/517 R, 73/517 B
• US Class Current: 310/316.01
• CPC Class Codes: G01N 2291/02827 Elastic parameters, strength or force
• CPC Class Codes: G01P 15/0907 of the compression mode type
• CPC Class Codes: G01P 15/0922 of the bending or flexing mode type
• CPC Class Codes: G01P 15/097 by vibratory elements

Abstract

An electronically tunable resonant accelerometer is shown wherein the frequency of a resonant peak may be adjusted over a range of frequencies. A piezoelectric element of the accelerometer is used with a seismic mass to generate an output voltage in response to reciprocating motion of the accelerometer. In a compression mode, a feedback loop applies a feedback voltage to a second piezoelectric element mechanically coupled to the first mentioned piezoelectric element. In a cantilever mode, a feedback loop applies a feedback voltage to another location along the first mentioned piezoelectric element which is formed from two bonded piezoelectric elements. By adjusting gain and phase of the feedback loop, first, the resonant frequency of the accelerometer may be varied over a wide range of frequencies to give increased sensitivity to reciprocating motion occurring at a frequency within a narrow band width centered on the resonant frequency, and, second, damping of the resonance may be varied to control the band width of the resonance.

Claims

1. An electronically tunable resonant accelerometer for measuring applied reciprocating motion within a predetermined frequency range comprising:

piezoelectric generating means for generating an output signal in response to said motion, said piezoelectric generating means having a resonant frequency;

means for amplifying said output signal;

feedback loop including means for adjusting gain of said feedback loop, and means for adjusting phase of a feedback signal from said amplifying means;

piezoelectric feedback means mechanically coupled to said piezoelectric generating means and receiving said feedback signal from said feedback loop, said gain adjusting means and said phase adjusting means being adapted to vary said feedback signal and thereby tune said resonant frequency of said piezoelectric generating means over said predetermined frequency range;

means for mounting said piezoelectric generating means and said feedback means and applying said reciprocating motion thereto.

2. The electronically tunable resonant accelerometer as given in claim 1 wherein said feedback loop comprises band pass means for allowing said feedback sigal within a band width about said resonant frequency to pass therethrough.

3. The electronically tunable resonant accelerometer as given in claim 2 wherein said band pass means includes high pass filter means for controlling a lower limit of said band width, and low pass filter means for controlling an upper limit of said band width.

4. The electronically tunable resonant accelerometer as given in claim 3 comprising means for damping said accelerometer to prevent unwanted oscillation of said accelerometer caused by said feedback signal and to vary a quality factor at resonance.

5. The electronically tunable resonant accelerometer as given in claim 4 wherein said amplifying means has a high input impedance and a low impedance output signal.

6. The electronically tunable resonant accelerometer as given in claim 4 further comprising inverter means in said feedback loop, said gain adjusting means being mechanically coupled to said phase adjusting means wherein varying of gain adjusting means simultaneously varies said phase adjusting means for said tuning of said resonant frequency over said frequency range.

7. The electronically tunable resonant accelerometer as given in claim 1 wherein said piezoelectric generating means is a first piezoelectric element and seismic mass, and said piezoelectric feedback means is a second piezoelectric element, said first and second piezoelectric elements operating in a compression mode.

8. The electronically tunable resonant accelerometer as given in claim 1 wherein said accelerometer is tuned on a high frequency side of said resonant frequency if said piezoelectric feedback menas is caused to change its dimensions in an opposite sense from a dimensional change of said piezoelectric generating means caused by said reciprocating motion, and on a low frequency side of said resonant frequency if said piezoelectric feedback means is caused to change its dimensions in a like sense to a dimensional change of said piezoelectric generating means caused by said reciprocating motion.

9. The electronically tunable resonant accelerometer as given in claim 1 wherein piezoelectric generating means and said feedback means are connected in a cantilever mode with two piezoelectric slabs being connected together along their longitudinal axis, said mounting means being on a first end of said two piezoelectric slabs.

10. The electronically tunable resonant accelerometer as given in claim 9 comprising first output electrode means connected to a first of said two piezoelectric slabs near said first end and second output electrode means connected to a second of said two piezoelectric slabs opposite said first output electrode means, said first and second output electrode means detecting said output signal, first feedback electrode means connected to said first piezoelectric slab at approximately the center of said longitudinal axis and second feedback electrode means connected to said second piezoelectric slab opposite said first feedback electrode means, said first and second feedback electrode means applying said feedback signal to said piezoelectric feedback means.

11. The electronically tunable resonant accelerometer as given in claim 10 comprising a seismic mass on a second end of said two piezoelectric slabs, said accelerometer being tunable on a high side of said resonant frequency if said piezoelectric feedback means is caused to change its dimensions in an opposite sense from a dimensional change of said piezoelectric generating means caused by said reciprocating motion, and on a low frequency side of said resonant frequency if said piezoelectric feedback means is caused to change its dimensions in a like sense to a dimensional change of said piezoelectric generating means caused by said reciprocating motion.

12. A method of tuning resonant frequency of an accelerometer over a frequency range consisting of the following steps:

mechanically coupling a first piezoelectric means to a second piezoelectric means;

amplifying an output signal generated by said first piezoelectric means in response to motion thereof;

connecting a feedback signal from said output signal through a feedback loop to said second piezoelectric means;

adjusting gain of said feedback loop and simultaneously varying phase of said feedback signal through said feedback loop;

said adjusting gain and varying phase tuning said resonant frequency over said frequency range.

13. The method of tuning resonant frequency of an accelerometer as recited in claim 12 includes an additional step of changing damping of said feedback loop.

14. The method of tuning resonant frequency of an accelerometer as recited in claim 13 includes a step of passing said feedback signal through a band pass filter, said band pass filter setting said frequency range.

15. The method of tuning resonant frequency of an accelerometer as recited in claim 14 wherein said frequency range is on a high frequency side of said resonant frequency if said piezoelectric feedback means is caused to change its dimensions in an opposite sense from a dimensional change of said piezoelectric generating means caused by said reciprocating motion.

16. The method of tuning resonant frequency of an accelerometer as recited in claim 14 wherein said frequency range is on a low frequency side of said resonant frequency if said piezoelectric feedback means is caused to change its dimensions in a like sense to a dimensional change of said piezoelectric generating means caused by said reciprocating motion.