Method of improving measurement speed of distributed optical fiber sensor by adopting orthogonal signals and system thereof

Patent metadata

Field	Value
Publication number	US-10564012-B2
Application number	US-201815874672-A
Country	US
Kind code	B2
Filing date	Jan 18, 2018
Priority date	Aug 8, 2017
Publication date	Feb 18, 2020
Grant date	Feb 18, 2020

Abstract

A method of improving measurement speed of distributed optical fiber sensors by adopting orthogonal signals and the system thereof is disclosed, which is related to the optical fiber sensor field and solves the problems that conventional technology will increasing the bandwidth of the received signal, reducing the signal-to-noise ratio of the received signal or distortion the spatial resolution of the system. The method comprises steps of generating N periodic orthogonal optical pulse sequence; injecting the N periodic orthogonal optical pulse sequence into the optical fiber under test( 5 ); collecting the scattered light signal; demodulating the scattered light signal with the local oscillating light and then converting into digital signals; extracting the scatter information of the orthogonal optical pulses from the collected digital signals; and arranging the scattered information in order of precedence of the infusion. The measurement speed of the distributed optical fiber sensors is improved by N−1 times.

First claim

What is claimed is:

1. A method of improving a measurement speed of distributed optical fiber sensors by adopting orthogonal signals, comprising steps of:
step 1: generating a periodic orthogonal optical pulse sequence; wherein one cycle contains N mutually orthogonal signals, and these orthogonal signals are coherently demodulated to share same detector bandwidth, wherein N denotes a total number of orthogonal signals
step 2: injecting the periodic orthogonal optical pulse sequence into an optical fiber under test in order of precedence and collecting scattered light signals; demodulating the scattered light signals with a local oscillating light, and transforming the demodulated signal into digital signals; and
step 3: extracting scatter information of each of orthogonal optical pulses of the periodic orthogonal optical pulse sequence from collected digital signals; arranging the scatter information in order of precedence of the injecting into the optical fiber under test.

2. A method of an electrical signal generating unit generating two channels of orthogonal electrical pulses with a frequency of f 1 named pulses-I and pulses-Q, comprising steps as follow:
generating two pulses with an initial phase of 0° and a delay of nL/c as pulses-I, wherein a math expression of an I channel-signal is written as:
V Ii ( t )= V D cos(2π f 1 t )rect( t/T )+ V D cos(2π f 1 t )rect[( t−nL/c )/ T ]

meanwhile, generating two pulses with initial phases of 90° and −90° respectively and a delay of nL/c as pulses-Q, wherein a math expression of a Q-channel signal is as below:
V Qi ( t )= V D cos(2π f 1 t+π/ 2)rect( t/T )+ V D cos(2π f 1 t−π/ 2)rect[( t−nL/c )/ T

wherein L denotes a length of the optical fiber under test; c denotes a speed of light in vacuum; n denotes a refractive index of an optical fiber under test; V D denotes a radio-frequency signal amplitude of a modulation; rect denotes a rectangular function; T denotes a pulse width; t denotes a time variable;
the pulses-I and pulses-Q are respectively used as the i-channel signal and the q-channel signal input IQ modulator to modulate the continuous-wave light, and a generated signal is expressed as
E i =E c cos[2π( f c +f 1 ) t ]rect( t/T )+ E c cos[2π( f c −f 1 ) t ]rect[( t−nL/c )/ T ]

wherein, f c denotes a frequency of an continuous-wave light; E c denotes a signal amplitude of an optical signal after modulation;
Ei is one period of a periodic orthogonal pulse sequence, the period of the periodic orthogonal pulse sequence is 2nL/c;
injecting the periodic orthogonal optical pulse sequence into an optical fiber under test in order of precedence and collecting scattered light signals;
demodulating the scattered light signals with a local oscillating light, a demodulated signal is as below:
E 0 =AR ( z )exp{ j [2π f 1 ( t−T z )−2π f c T z ]}·rect[( t−T z )/ T ]+ AR ( z )exp{− j [2π f 1 ( t−T z )+2π f c T z ]}·rect[( t−nL/c−T z )/ T ]

wherein, j denotes an imaginary unit; A denotes a response factor of a probe; T z denotes a delay of receiving a scattered light signal on point z on the optical fiber under test at a receiver; R(z) denotes a distribution of a scattered light signal amplitude along the optical fiber under test;
transforming the demodulated signal into digital signals; wherein
the demodulated signal E 0 contains two parts of signal, and it can be divided in to frequency domain;
extracting scatter information of each of the orthogonal optical pulses of the periodic orthogonal optical pulse sequence from collected digital signals in the frequency domain; and
arranging the scatter information in order of precedence of the injecting into the optical fiber under test.

Assignees

• Univ Electronic Sci & Tech China

Inventors

• Wang Zinan
• Xiong Ji
• Xie Lianlian
• Rao Yunjiang

Classifications

• G01P3/36 Primary

  Devices characterised by the use of optical means, e.g. using infrared, visible, or ultraviolet light (G01P3/68 takes precedence; gyrometers using the Sagnac effect, i.e. rotation-induced shifts between counter-rotating electromagnetic beams G01C19/64) · CPC title

• G01D5/353 Primary

  influencing the transmission properties of an optical fibre · CPC title

• G01D5/35358

  using backscattering to detect the measured quantity · CPC title

• G01D5/268

  using optical fibres (G01D5/28 - G01D5/38 take precedence) · CPC title

• G01D5/35335 Primary

  Aspects of emitters or receivers used by an interferometer in an optical fibre sensor arrangement (using multiple sensor devices using multiplexing techniques G01D5/35383) · CPC title