Complex structural component defect optical fiber acoustic detection system and detection and imaging method thereof
A detection system, optical fiber acoustic technology, applied in measuring devices, using sound waves/ultrasonic waves/infrasonic waves to analyze solids, using sound waves/ultrasonic waves/infrasonic waves for material analysis, etc., can solve inaccurate positioning, affect probe sensitivity, and sound field energy transmission loss and other problems, to achieve the effects of high detection accuracy, fast computing and imaging speed, and high sensitivity
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specific Embodiment approach 1
[0044] Specific Embodiment 1: In this embodiment, the optical fiber acoustic detection system for defects in complex structural parts includes an ultrasonic transducer array, an optical fiber sensing signal detection and demodulation system, and a computer imaging system; it is characterized in that:
[0045] The ultrasonic transducer array is fabricated as a fan-shaped phased array;
[0046] The optical fiber sensing signal detection and demodulation system includes a light source, a wavelength division multiplexer, a fiber laser sensor array, an unbalanced Michelson fiber interferometer, and a photodetector; the unbalanced Michelson fiber interferometer uses 2×2 couplers, 3×3 Composed of a coupler and a Faraday rotating mirror; the fiber laser sensor array is composed of four DFB lasers connected in series, the four DFB lasers share one optical path, and the four DFB lasers are arranged in a square.
[0047] In this embodiment, the pump laser enters four DFB lasers (distribu...
specific Embodiment approach 2
[0068] Embodiment 2: The difference between this embodiment and Embodiment 1 is that the length of the DFB laser is 5 cm. Other steps and parameters are the same as those in Embodiment 1.
[0069] In order to facilitate single longitudinal mode laser oscillation and facilitate packaging, this embodiment adopts a distributed feedback laser (DFB) with a length of 5 cm. It can be seen from formula (A1) that the change of the effective refractive index of the core region of the erbium-doped fiber or the change of the grating period will lead to the change of the operating wavelength of the DFB laser. When the DFB laser is subjected to external sound pressure, the strain generated by the sound pressure will change the effective refractive index of the fiber and the period of the grating. At this time, the change in the operating wavelength of the DFB laser can be determined by the following formula:
[0070]
[0071] where P 11 and P 12 is the photoelastic coefficient, ε z ,...
specific Embodiment approach 3
[0080] Embodiment 3: The difference between this embodiment and Embodiment 1 or 2 is that the side length of the squares arranged by DFB lasers is 8-20 cm. Other steps and parameters are the same as those in Embodiment 1 or 2.
[0081] The sound wave will attenuate when it propagates in the medium. During the propagation process, due to the diffusion of the wave front, the energy space will be diffused, so that the wave amplitude will attenuate with the increase or decrease of the distance. This attenuation is called geometric attenuation. Due to the scattering effect of the particles in the medium, the energy of the sound wave in the original propagation direction is reduced, resulting in a significant attenuation of the wave amplitude with the increase of the propagation distance. The loss of sound waves in the medium includes the dissipation caused by viscous force, heat conduction and relaxation process. Heat conduction dissipation is due to the fact that during the propa...
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