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Dual-wavelength nonlinear displacement demodulation method and system of optical fiber Fabry-Perot displacement sensor

A displacement sensor and demodulation system technology, applied in the field of optical fiber sensing, can solve the problems of large positive displacement demodulation error, large negative displacement demodulation error, small measurement range, etc., to prevent the interference of invalid measurement, accurate High performance, compact structure

Active Publication Date: 2019-08-13
CHONGQING UNIV
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

When the optical fiber Fabry-Perot displacement sensor measures vibration displacement, it mainly faces three problems: 1) The measurement range is small, and it is easy to exceed the range for large displacement measurement
3) Perform nonlinear displacement demodulation by modifying the working wavelength of the laser. If the wavelength is set close to the trough of the reflection spectrum, the positive displacement can be demodulated well, but the demodulation error of the negative displacement is large; if the wavelength is set close to the peak of the reflection spectrum, the negative The displacement in the direction can be demodulated very well, but the demodulation error in the forward displacement is large

Method used

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  • Dual-wavelength nonlinear displacement demodulation method and system of optical fiber Fabry-Perot displacement sensor

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Embodiment 1

[0038] Embodiment 1: Dual-wavelength nonlinear displacement demodulation system of optical fiber Fabry-Perot displacement sensor

[0039] see figure 1 , the system includes: a PC 101, a first wavelength tunable laser 102, a second wavelength tunable laser 103, a first fiber coupler 106, a fiber circulator 108, a fiber Fabry-Perot displacement sensor 110, a second fiber coupler 113 , wavelength division multiplexer 116 , first photodetector 119 , second photodetector 120 , output terminal 121 , data acquisition card 122 and so on.

[0040] Adjust the optical fiber Fabry-Perot displacement sensor 110 so that its light emitting surface is parallel to the measured object 111 . When the measured object 111 is not vibrating, two channels of reflection spectrum signals are acquired. The first wavelength tunable laser 102, the second photodetector 120 and the data acquisition card work first to obtain the reflection spectrum of the optical fiber Fabry-Perot displacement sensor; the ...

Embodiment 2

[0045] Embodiment 2: Dual-wavelength nonlinear displacement demodulation system of optical fiber Fabry-Perot displacement sensor

[0046] see figure 2 , the system includes: a PC 201, a first wavelength tunable laser 202, a second wavelength tunable laser 203, a fiber coupler 206, a fiber circulator 208, a fiber Fabry-Perot displacement sensor 210, a wavelength division multiplexer 213, A first photodetector 216, a second photodetector 217, an output terminal 218, a data acquisition card 219, and the like.

[0047] Adjust the optical fiber Fabry-Perot displacement sensor 210 so that its light emitting surface is parallel to the measured object 211 . When the measured object 211 is not vibrating, two channels of reflection spectrum signals are acquired. The first wavelength tunable laser 202, the first photodetector 216, the wavelength division multiplexer 213 and the data acquisition card work earlier to obtain the reflection spectrum of the optical fiber Fabry-Perot displa...

Embodiment 3

[0052] Embodiment 3: Dual-wavelength nonlinear displacement demodulation method of optical fiber Fabry-Perot displacement sensor

[0053] This embodiment is a method for the dual-wavelength nonlinear displacement demodulation system applied to the above-mentioned optical fiber Fabry-Perot displacement sensor, below in conjunction with the attached image 3 The steps of this method are described in further detail.

[0054] Step 1. Obtain two reflection spectrum signals: when the measured object 211 is not vibrating, the first wavelength tunable laser 202, the first photodetector 216 and the data acquisition card 219 are working, and the obtained optical fiber Fabry-Perot displacement sensor 210 first A reflection spectrum curve, such as Figure 4 Shown; Then the second wavelength tunable laser 203, the second photodetector 217 and the data acquisition card 219 work, the second road reflection spectrum curve of the optical fiber Fabry-Perot displacement sensor 210 that obtains,...

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Abstract

The invention discloses a dual-wavelength nonlinear displacement demodulation method and system of optical fiber Fabry-Perot displacement sensor, belonging to the technical field of optical fiber sensing. The system comprises an optical fiber Fabry-Perot displacement sensor, two paths of wave length tunable lasers, two optical fiber couplers, an optical fiber circulator, a wavelength division multiplexer, two photoelectric detectors and a data collection card. The method comprises the following steps of: 1) acquiring two paths of reflectance spectrums; 2) setting working wavelengths of the twopaths of lasers, and respectively determining initial phases; 3) performing phase conversion of the reflection spectrums, curve fitting and solving of an inverse function; 4) calculating the change quantity of the optical phase, and determining the change quantity of the cavity length; 5) and demodulating the nonlinear displacement according to the model. The dual-wavelength nonlinear displacement demodulation method and system can improve the measuring range of the traditional optical fiber Fabry-Perot displacement sensor, are high in demodulation precision, can overcome the problem of fuzzyphase, are flexible in demodulation, and can give evaluation for the reliability of the demodulation result.

Description

technical field [0001] The invention belongs to the technical field of optical fiber sensing, and in particular relates to the displacement demodulation technology of an optical fiber Fabry-Perot displacement sensor. Background technique [0002] With the development of science and technology, the monitoring and measurement of tiny vibrations in complex environments is becoming more and more important. However, the commonly used Doppler vibrometers, strain gauges, optical fiber displacement sensors and other instruments for measurement cannot adapt to the measurement methods. The measurement of complex environments or the inability to achieve high-precision micro-vibration measurement or the measurement of a large vibration range cannot be met. As a sound field calculation method, Rayleigh integration can calculate the sound pressure at any point in the field as long as the vibration velocity distribution on the surface of the transducer is measured. In the measurement envi...

Claims

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Application Information

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IPC IPC(8): G01B11/02
CPCG01B11/02
Inventor 王代华王杰吴轲卢文义
Owner CHONGQING UNIV
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