A dynamic pressure detection system and method based on fiber grating Stokes parameters
A fiber grating and dynamic pressure technology, applied in the direction of measuring force, measuring the change of optical properties of the material when it is stressed, measuring devices, etc., can solve problems such as poor real-time performance and difficult detection
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example 1
[0039] [Example 1] Design grating parameters: period Λ = 535nm, fiber core refractive index n eff =1.448, length L=10mm, refractive index modulation coefficient δn=1×10 -4 . The motorized polarization controller 3 is adjusted by the feedback module 7 so that the polarization state of the incident light is linearly polarized at 45°. Select the tunable laser wavelength λ=1549.3nm. When the sensing fiber grating 4 is affected by external pressure, the birefringence of the line will change, which will lead to the change of the three Stokes parameters of the transmitted light. The transmitted light passes through the online polarization analysis module 5 to detect the change of the polarization parameter, passes through the signal processing module 6, and displays three Stokes parameter values in the display module 8 to monitor the dynamic pressure received in real time. In this example, the theoretical relationship between the three Stokes parameters and the external pressure...
example 2
[0040] [Example 2] Design grating parameters: period Λ = 535nm, fiber core refractive index n eff =1.448, length 20mm, refractive index modulation coefficient δ n =1×10 -4 . Adjust the motorized polarization controller 3 to select multiple incident ray polarization angles, which are 30°, 45° and 60° respectively. In this example, the theoretical relationship between the variation of the three Stokes parameters and the external pressure under different incident polarization states is as follows image 3 As shown, the sensitivity, dynamic range, and linearity of the three Stokes parameters vary with the incident angle.
example 3
[0041] [Example 3] Actual grating parameters: length L=10mm, center wavelength 1550.06nm, maximum insertion loss 9dB. The tunable laser wavelength λ=1549.7nm. Initial incident polarization state (0.541, 0.244, 0.822). In this example, the vibration source pressed on the grating has a vibration period of 4.5ms and a frequency of about 222Hz. In this example, the monitored three Stokes parameters vary with dynamic pressure as Figure 4 As shown, the three Stokes parameters all have good responses to dynamic pressure.
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