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 cannot be demodulated, and the phase information demodulation of the disturbance signal cannot be realized. , to achieve the effect of improving the signal-to-noise ratio and increasing the optical power
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Embodiment 1
[0017] An optical fiber distributed acoustic wave monitoring system, which uses the frequency-modulated DFB fiber laser output narrow-linewidth, frequency-modulated laser as the laser light source of the optical fiber distributed acoustic wave monitoring system, and is characterized in that the laser output by the frequency-modulated DFB fiber laser enters the The acousto-optic modulator, through the acousto-optic modulator, the continuous laser is modulated into a pulsed laser with a pulse width of τ and a period of T. 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 end, the unit pulse laser passes through the C of the second circulator 22 Injection into a sensing fiber with a length of L will excite Rayleigh scattered light within the range of the unit length of the sensing fiber that the unit pulse laser passes through. Because the pulse laser with narrow linewidth has good co...
Embodiment 2
[0045] The similarities between this embodiment and Embodiment 1 will not be repeated, as Figure 8 As shown, the difference from Embodiment 1 is that the back Rayleigh scattering interference is formed in a different way. In this embodiment, the B of the fifth coupler is used. 53 , B 54 The Michelson interferometer with arm length difference S formed at both ends interferes the back Rayleigh scattering signals between different unit lengths. The back Rayleigh scattering signal output by the second optical filter enters the C of the third circulator 31 terminal, from the C of the third circulator 32 end flows into the fifth coupler's B 51 end, through the fifth coupler beam splitting to B 53 and B 54 end, B 53 and B 54 The two ends constitute a Michelson interferometer with arm length difference, B 53 The length of the light at the end is L 1 The optical fiber is reflected by the third Faraday rotating mirror and returns to the fifth coupler B 53 end, B 54 The lengt...
Embodiment 3
[0048] The similarities between this embodiment and Embodiment 1 will not be repeated, as Figure 9 As shown, the difference from Embodiment 1 is that the interference forming method of interfering the back Rayleigh scattering signals between different unit lengths on a sensing fiber using an interferometer is different. In this embodiment, The seventh coupler and the time-delay fiber are the main components to form a time-delay ring Sagnac interferometer to interfere the back Rayleigh scattering signals between different unit lengths.
[0049] Said using the seventh coupler and 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 scattering signal output by the second optical filter The scattered signal enters the B of the sixth coupler 61 end, through the beam splitting of the sixth coupler, all the light enters the C of the fourth circulator...
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