Fiber-Perot water hearing device arbitrarily non-linear sound pressure demodulation method and system
A technology of nonlinear acoustic and demodulation methods, applied in instruments, measuring ultrasonic/sonic/infrasonic waves, measuring devices, etc., can solve the problems of uncertain phase increase or decrease, large calculation error, phase ambiguity, etc., and achieve linearity Good accuracy, simple demodulation system, good repeatability
- Summary
- Abstract
- Description
- Claims
- Application Information
AI Technical Summary
Problems solved by technology
Method used
Image
Examples
Embodiment 1
[0036] Example 1: Nonlinear Sound Pressure Demodulation System at Any Working Point of Optical Fiber Fabry-Perot Hydrophone
[0037] see figure 1 The structure of the optical fiber Fabry-Perot hydrophone involved in the nonlinear sound pressure demodulation method at any working point of the optical fiber Fabry-Perot hydrophone provided by the present invention includes: input / output single-mode optical fiber 003, reflective optical fiber 001 and quartz capillary 002, The two ends of the quartz capillary are respectively fused with the single-mode optical fiber and the reflective optical fiber, and the air cavity in the quartz tube is used as an interference cavity; an optical fiber Fabry-Perot hydrophone is naturally formed between the two reflective surfaces of the air cavity Fabry-Perot cavity of the device.
[0038] figure 2Shown is a schematic diagram of the system structure of an embodiment of the method for demodulating the nonlinear sound pressure at any working poi...
Embodiment 2
[0039] Embodiment 2: Demodulation method of nonlinear sound pressure at any working point of optical fiber Fabry-Perot hydrophone
[0040] image 3 The flow chart of the demodulation method for this system includes the following steps:
[0041] 1. Obtain the reflection spectrum: the ultrasonic transducer 107 does not output to ensure that the ultrasonic wave does not act on the optical fiber Fabry-Perot hydrophone 106, and the data acquisition card 110 records the output voltage V of the photodetector 109 along with the wavelength of the tunable laser 102 wavelength Discrete point data, i.e. reflectance spectrum, with increasing λ variation, such as Figure 4 shown. Then the ultrasonic transducer 107 outputs the ultrasonic wave to act on the fiber optic Fabry-Perot hydrophone.
[0042] 2. Adjust the working point of the laser and determine the initial phase: 101 pairs of PCs Figure 4 The mid-reflection spectrum is subjected to Fourier transform, the cavity length L of the...
PUM
Login to View More Abstract
Description
Claims
Application Information
Login to View More 


