1994
DOI: 10.1177/014233129401600204
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A practical optical force-feedback microphone

Abstract: A novel technique of measuring diaphragm displacement in microphones using a laser-diode Fabry-Perot system is presented. The microphone diaphragm is held within an electrostatic force-feedback loop so as to improve the performance. A second loop operates around the laser, for noise minimisation purposes. Following a brief introduction to the subject of optical detection in microphones, the modified Fabry-Perot interferometer is described, and the complete system with the two feedback loops presented. The cha… Show more

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Cited by 7 publications
(4 citation statements)
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“…The system in ( 7) displays a damped oscillatory response, which is typical of many feedback-controlled transduction processes encountered in cantilever positioning in atomic force microscopy, 93 optical force feedback microphones, [94][95][96] or the control of complex deexcitation lifetimes encountered in many types of spectroscopies, e.g., nuclear magnetic, 97 electron-spin, 98,99 microwave, [100][101][102] and multiphoton fluorescence, e.g., Förster resonance, 103 and in lock-in applications 104 or in other control and identification schemes. 105 The desired closed-loop dynamics are specified in the form (6) with aD = bD = 0.5, which corresponds to a first-order transfer function with a time constant of 2 s. All the simulations were carried out by using the Matlab ® /Simulink ® software and the FOTF code 106 for fractional-order systems available within the FOMCON toolbox (www.fomcon.net).…”
Section: Preliminary Examplementioning
confidence: 99%
“…The system in ( 7) displays a damped oscillatory response, which is typical of many feedback-controlled transduction processes encountered in cantilever positioning in atomic force microscopy, 93 optical force feedback microphones, [94][95][96] or the control of complex deexcitation lifetimes encountered in many types of spectroscopies, e.g., nuclear magnetic, 97 electron-spin, 98,99 microwave, [100][101][102] and multiphoton fluorescence, e.g., Förster resonance, 103 and in lock-in applications 104 or in other control and identification schemes. 105 The desired closed-loop dynamics are specified in the form (6) with aD = bD = 0.5, which corresponds to a first-order transfer function with a time constant of 2 s. All the simulations were carried out by using the Matlab ® /Simulink ® software and the FOTF code 106 for fractional-order systems available within the FOMCON toolbox (www.fomcon.net).…”
Section: Preliminary Examplementioning
confidence: 99%
“…For example, the Doppler frequency shift of light reflected from a microphone membrane is used to measure the membrane's velocity in [13]. A Fabry-Perot cavity was incorporated into the interferometers used in [14,15]. In the latter study, a Pockel's cell is used for highspeed switching between interference signals with a fixed 90 • phase difference.…”
Section: Introductionmentioning
confidence: 99%
“…With the exception of [11,14], each of the optical microphones discussed above is operated in an open loop, in other words without the presence of feedback. In a feedback-controlled microphone, a control loop is integrated into the sensor in order to detect and nullify the microphone's membrane deflection, caused by the sound pressure, using an opposing pressure that is produced by electrostatic, electromagnetic or other electrical means.…”
Section: Introductionmentioning
confidence: 99%
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