Abstract

Distributed optical fiber sensors (DOFSs) have faced the challenge of measuring transverse stress along the fiber and the current main approach has been based on polarization coupling effect in polarization-maintaining fibers (PMFs), which has short sensing length and high dependence on direction of exerted stress. Instead, here we propose a novel distributed transverse stress sensor (DTSS) based on coupling effect between linearly-polarized (LP) modes in weakly-coupled few-mode-fibers (FMFs). In this scheme, multiple LP modes could be considered as independent spatial channels without stress perturbation because of ultralow inherent modal crosstalk, while quantifiable and spatially-resolvable mode coupling for a probe signal will occur under transverse stress satisfying phase-matching conditions. A proof-of-concept DTSS system is verified based on weakly-coupled two-mode fibers and mode-selective couplers for mode conversion. Moreover, we show that the scheme is little affected by mild common parameters including temperature, strain, twist, direction of stress, or state-of-polarization (SOP), which is crucial for accurate stress analysis under complex environmental conditions. The proposed DTSS scheme has simple structure, high flexibility for different sensing ranges and resolutions, and high collaborating capability with other sensing mechanisms.

Highlights

  • In recent years, distributed optical fiber sensors (DOFSs) utilizing the entire fiber as both the sensing element and transmission medium have experienced an explosive growth [13], in which intensity, phase, or frequency changes of probe light caused by a specific parameter under investigation along the fiber can be detected with spatial resolution

  • We propose a novel distributed transverse stress sensor (DTSS) mechanism based on linearly-polarized (LP) mode coupling effect under transverse stress in weakly-coupled few-mode fibers (FMFs), which is quite different with previous studies for DOFSs over FMFs such as monitoring multiple parameters simultaneously with multiple LP modes or improving system performance utilizing transmission characteristics of FMFs [15]

  • Step-index circular-core (SI-CC) two-mode fiber (TMF) removed of the coating is subjected to a small transverse stress in the y-axis, the fiber core will suffer from the slight effects including birefringence, elliptical deformation, and displacement perturbation [17], among which only displacement perturbation is important because coupling can only occur between two LP modes when their azimuthal orders differ by ±2 for elliptical deformation and that is dissatisfied in TMFs [22], and birefringence can only cause coupling between the polarization components of one mode and we only consider the superposition of them [22]

Read more

Summary

INTRODUCTION

In recent years, distributed optical fiber sensors (DOFSs) utilizing the entire fiber as both the sensing element and transmission medium have experienced an explosive growth [13], in which intensity, phase, or frequency changes of probe light caused by a specific parameter under investigation along the fiber can be detected with spatial resolution. Distributed transverse stress sensors (DTSSs) have been little studied, which could find unique applications in many fields such as geological disaster monitoring and early warning, structural health monitoring, medical monitoring, manufacturing process monitoring, and so on [7], especially in pressure monitoring area, including oil/gas downhole and pipeline, geotechnical engineering, water distribution and sewerage utilities [8, 9]. In these cases, the sensing of transverse stress is more effective and cannot be replaced by other sensing mechanisms. Step-index circular-core (SI-CC) TMF removed of the coating is subjected to a small transverse stress in the y-axis, the fiber core will suffer from the slight effects including birefringence, elliptical deformation, and displacement perturbation [17], among which only displacement perturbation is important because coupling can only occur between two LP modes when their azimuthal orders differ by ±2 for elliptical deformation and that is dissatisfied in TMFs [22], and birefringence can only cause coupling between the polarization components of one mode and we only consider the superposition of them [22]

PRINCIPLE OF OPERATION
EXPERIMENTAL SETUP AND RESULTS
CONCLUSIONS
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call