A Method of Measuring Electrostrictive Coefficient by Linear Frequency Modulation Multi-beam Laser Heterodyne
A technology of linear frequency modulation and laser heterodyne, which is applied in the field of ultra-precision measurement, can solve the problems of low measurement accuracy and achieve the effects of large measurement range, low power consumption, and high spatial and temporal resolution
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specific Embodiment approach 1
[0023] Specific implementation mode one: combine figure 1 Describe this embodiment, the device for chirp multi-beam laser heterodyne measurement of electrostriction coefficient described in this embodiment includes a chirp laser 1, a photodetector 3, a converging lens 4, a thin glass plate 5, and a No. 2 plane mirror 6 and adjustment frame 8;
[0024] The adjustment frame 8 is used to fix the piezoelectric body 7 to be tested, and the No. 2 plane reflector 6 is used to be fixed on an end face of the piezoelectric body 7 to be tested. The glass plate 5 is arranged parallel to the No. 2 plane reflector 6;
[0025] The laser light emitted by the chirp laser 1 is incident on the surface of the thin glass plate 5, and the laser light transmitted through the thin glass plate 5 is incident on the second plane reflector 6, and between the second plane reflector 6 and the thin glass plate 5 Multiple reflected light beams are obtained after multiple reflections, and the multiple refle...
specific Embodiment approach 2
[0029] Specific implementation mode two: combination figure 1 Describe this embodiment. This embodiment is a further limitation of the device for measuring the electrostrictive coefficient by chirp multi-beam laser heterodyne described in Embodiment 1. In this embodiment, the chirp multi-beam laser heterodyne measurement The device of the electrostriction coefficient also includes a signal processing system 2, the detection signal input end of the signal processing system 2 is connected to the detection signal output end of the photodetector 3, and the signal processing system 2 includes a filter 2-1, a front Amplifier 2-2, A / D converter 2-3 and DSP2-4, the signal input end of the filter 2-1 is the detection signal input end of the signal processing system 2, the filter 2-1 The signal output terminal is connected to the signal input terminal of the preamplifier 2-2, and the signal output terminal of the preamplifier 2-2 is connected to the analog signal input terminal of the A...
specific Embodiment approach 3
[0031] Specific implementation mode three: combination figure 1 Describe this embodiment. This embodiment is a further limitation of the device for measuring the electrostrictive coefficient by chirp multi-beam laser heterodyne described in Embodiment 1. In this embodiment, the chirp multi-beam laser heterodyne measurement The electrostrictive coefficient device also includes a No. 1 plane reflector 10 , and the laser light emitted by the chirp laser 1 is reflected by the No. 1 plane reflector 10 and then incident on the surface of the thin glass plate 5 .
[0032] In this embodiment, a No. 1 plane reflector 10 is arranged between the chirp laser 1 and the thin glass plate 5. The No. 1 plane reflector 10 reflects the laser light emitted by the chirp laser 1, and the reflected light is incident on the thin glass plate. 5 surfaces. During measurement, the incident angle of the laser light on the thin glass plate 5 can be adjusted by adjusting the angle of the No. 1 flat mirror ...
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