基于有源多芯光纤光栅的拍频传感结构及二维矢量传感方法

By using a beat frequency sensing structure composed of active multi-core fiber optic gratings and a two-dimensional vector sensing method, the problem of measuring weak seismic wave signals in deep oil and gas exploration has been solved, achieving high-sensitivity and high-resolution seismic wave signal detection, and enabling the detection of seismic wave vibration acceleration with μg-level resolution.

CN119620160BActive Publication Date: 2026-07-17NORTHWEST UNIV

Patent Information

Authority / Receiving Office
CN · China
Patent Type
Patents(China)
Current Assignee / Owner
NORTHWEST UNIV
Filing Date
2024-11-29
Publication Date
2026-07-17

AI Technical Summary

Technical Problem

Existing fiber Bragg grating sensors are difficult to accurately measure weak seismic wave signals in deep oil and gas exploration, especially when the wavelength shift is less than 0.02 nm. Traditional spectrometers cannot achieve accurate measurement and have insufficient sensitivity and resolution.

Method used

A beat frequency sensing structure composed of active multi-core fiber gratings is adopted. By writing gratings with different reflectivities on multi-core optical fibers to form an FP resonant cavity, energy is provided by a pump light source to form a single-frequency laser channel, and the magnitude and azimuth of the vibration signal are obtained by the beat frequency signal, which is converted into frequency difference component measurement.

Benefits of technology

It improves the measurement accuracy and sensitivity of weak seismic wave signals, enabling the detection of seismic wave vibration acceleration signals with μg-level resolution. The sensitivity is improved by three orders of magnitude, achieving high-resolution seismic wave signal detection.

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Abstract

基于有源多芯光纤光栅的拍频传感结构及二维矢量传感方法,该传感结构包括七芯有源多芯光纤,有源多芯光纤中除中心纤芯外、4根以上的偶数根、呈中心对称分布的纤芯的第一位置上均刻写有第一光栅、第二位置上均第二光栅,同一根纤芯上第一光栅和第二光栅的反射率不同,构成F‑P谐振腔,用于放大或反射特定波长的光,使每个纤芯变为单频激光通道,当F‑P谐振腔感受到地震波信号产生形变时,通过纤芯的激光就发生变化,呈中心对称的两个单频激光通道即可实现拍频,任意选取至少两组拍频信号,通过频率计数器测量拍频值,通过分析拍频信号的频率变化来获取振动信号的大小,通过选取的单频激光通道的几何位置关系得到振动信号的方位角。
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