Optical fiber distributed type sound wave monitor system
A fiber optic distributed, monitoring system technology, applied in the direction of measuring ultrasonic/sound wave/infrasonic wave, measuring device, using wave/particle radiation, etc., can solve the problems that the phase information demodulation of the disturbance signal cannot be realized, and the phase information cannot be demodulated. , to achieve the effect of increasing the optical power and improving the signal-to-noise ratio
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Embodiment 1
[0017] An optical fiber distributed acoustic wave monitoring system, which uses the narrow linewidth and frequency-modulated laser output from the frequency-modulated DFB fiber laser as the laser light source of the fiber-optic distributed acoustic wave monitoring system, characterized in that the laser output from the frequency-modulated DFB fiber laser enters the The acousto-optic modulator modulates the continuous laser into a pulsed laser with a pulse width of τ and a period of T through the acousto-optic modulator. The pulsed laser passes through the first optical amplifier and the first optical filter in turn and then enters the C of the second circulator. 21 terminal, the unit pulse laser passes through the C of the second circulator 22 Injecting a sensing fiber with a length of L into the end will excite Rayleigh scattered light within the range of the sensing fiber of unit length passed by the unit pulse laser. Lee scattered light in the second circulator C 23 interf...
Embodiment 2
[0045] The same points between this embodiment and Embodiment 1 will not be repeated here, such as Figure 8 As shown, the difference from Embodiment 1 is that the back Rayleigh scattering interference formation method is different. In this embodiment, the B of the fifth coupler is used. 53 , B 54 A Michelson interferometer with arm length difference S formed at both ends interferes the back-Rayleigh scattering signals between different unit lengths. The back-Rayleigh scattered signal output by the second optical filter enters the C of the third circulator 31 end, from the C of the third circulator 32 terminal flows out into the B of the fifth coupler 51 end, through the fifth coupler beam split to B 53 and B 54 end, B 53 and B 54 The two ends form a Michelson interferometer with arm length difference, B 53 The light at the end passes through a length L 1 The fiber is reflected back to the fifth coupler B by the third Faraday rotating mirror 53 end, B 54 The light a...
Embodiment 3
[0048] The same points between this embodiment and Embodiment 1 will not be repeated here, such as Figure 9 As shown, the difference from Embodiment 1 is that the interference formation method of interfering the back-Rayleigh scattering signals between different unit lengths on a sensing fiber by using an interferometer is different. The seventh coupler and the time-delay fiber are the main components to form a time-delay loop Sagnac interferometer to interfere the back-Rayleigh scattering signals between different unit lengths.
[0049] The use of the seventh coupler and the delay fiber as the main components to form a delay ring Sagnac interferometer to interfere the back-Rayleigh scattering signals between different unit lengths refers to the back-Rayleigh output of the second optical filter. Benefit the scattered signal into the B of the sixth coupler 61 end, through the beam splitting of the sixth coupler, one light enters the C of the fourth circulator 41 end, by the ...
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