Optical fiber Fabry-Perot sensor multiplexing method and device based on multi-wavelength and low-coherence light source
A method of Faber sensor and multiplexing device, applied in the field of fiber Faber sensor multiplexing method and device, to achieve the effect of not affecting demodulation accuracy and stability, reducing cost, and independent demodulation
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Embodiment 1
[0027] Example 1: Multiplexing device for optical fiber F-P sensor based on multi-wavelength low-coherence light source
[0028] The device consists of a light source module, a 3dB coupler, a fiber optic sensor, a multi-channel beam combiner, a demodulation interferometer, a photoelectric conversion device, an acquisition card, and a computer. Multimode optical fibers are used between the components of the optical path for optical signal transmission. :
[0029] The light source module 1 is composed of a broadband light source 2 and N first and second filters of different wavelengths...i-th filter and N-th filter, and the light emitted by the broadband light source 2 is coupled into N multimode optical fibers 7 at the same time , N represents the total number of multiplexing channels of the optical fiber Fab sensor. The broadband light of the i-th channel (i represents a number between 1 and N) passes through the i-th optical filter, and outputs low-coherent light with a wavele...
Embodiment 2
[0039] Example 2: Superposition analysis of low-coherence interference signals generated by multi-wavelength low-coherence light sources
[0040] Low-coherence interference refers to the use of a short coherence length light source to generate interference. It has the characteristics of the maximum interference fringe visibility when the optical path difference is zero, and with the increase and decrease of the optical path difference, the interference fringe visibility gradually decays. When the optical path difference is greater than the coherence length of the light source, the interference fringe visibility will be zero. It can be concluded that when the optical path difference is zero, it corresponds to the low coherence interference fringe envelope peak. This conclusion is based on low-coherence interferometry.
[0041] The multiplexing method of the present invention will be analyzed in detail below by taking the multiplexing of the four-channel optical fiber F-P senso...
Embodiment 3
[0047] Embodiment 3: Multiplexing method of optical fiber Fab sensor based on multi-wavelength low-coherence light source
[0048] The reflected light signals of the sensors of each channel are synthesized into a beam of light by the multi-channel beam combiner 17, and after being incident on the demodulation interferometer 18, the superposition result 38 of low-coherence interference fringes is output. The normalized light intensity function of superimposed low-coherence interference fringes is expressed as:
[0049] I ( λ , t ) = Σ i = 1 4 ∫ - ∞ + ∞ S i ( λ ) · I i ...
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