Measurement Using A Multi-Core Optical Fiber
US-2016018245-A1 · Jan 21, 2016 · US
US2018023948A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2018023948-A1 |
| Application number | US-201715646820-A |
| Country | US |
| Kind code | A1 |
| Filing date | Jul 11, 2017 |
| Priority date | Jul 19, 2016 |
| Publication date | Jan 25, 2018 |
| Grant date | — |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A Brillouin-based distributed bend fiber sensor and method for using the Brillouin-based distributed bend fiber sensor are described herein. In one example, the Brillouin-based distributed bend fiber sensor is specially configured to measure a temperature distribution (ΔT), a bend angle β, and a bend radius R along a deployed fiber (e.g., four-core fiber).
Opening claim text (preview).
1 . A Brillouin-based distributed fiber sensor comprising: a fiber comprising a first core, a second core, a third core, and a fourth core, wherein the first core, the second core, and the third core are located at three different positions along a circular path within the fiber, wherein the circular path has a radius (r) to a center of the fiber, and wherein the fourth core is located at the center of the fiber; and, a Brillouin backscattering sensing mechanism coupled to the first core, the second core, the third core, and the fourth core. 2 . The Brillouin-based distributed fiber sensor of claim 1 , further comprising: a processing system, coupled to the Brillouin backscattering sensing mechanism, configured to: obtain, prior to deployment of the fiber when the fiber has no bend applied thereto, from the Brillouin backscattering mechanism a first Brillouin frequency shift (BFS) baseline measurement (v B1 ) along the first core, a second BFS baseline measurement (v B2 ) along the second core, a third BFS baseline measurement (v B3 ) along the third core, and a fourth BFS baseline measurement (v B4 ) along the fourth core; obtain, after deployment of the fiber and when there is a bend applied to the fiber, from the Brillouin backscattering mechanism a first BFS bend measurement (v′ B1 ) along the first core, a second BFS bend measurement (v′ B2 ) along the second core, a third BFS bend measurement (v′ B3 ) along the third core, and a fourth BFS bend measurement (v′ B4 ) along the fourth core; calculate a change of a first, second, third, and fourth BFS distribution (Δv B1 , Δv B2 , Δv B3 , Δv B4 ) respectively along the first, second, third, and fourth cores; calculate a temperature distribution (ΔT) along the deployed fiber; calculate a first, second, and third bend induced strain distributions (Δε 1 , Δε 2 , Δε 3 ,) respectively along the first, second, and third cores; calculate a bend angle β along the deployed fiber; and calculate a bend radius R along the deployed fiber. 3 . The Brillouin-based distributed fiber sensor of claim 2 , wherein the processing system is further configured to calculate the change of the first, second, third, and fourth BFS distribution (Δv B1 , Δv B2 , Δv B3 , Δv B4 ) using the following equations: Δ v B1 =v B1 −v B1 ; Δ v B2 =v B2 −v B2 ; Δ v B3 =v B3 −v B3 , and, Δ v B4 =v B4 −v B4 . 4 . The Brillouin-based distributed fiber sensor of claim 2 , wherein the processing system is further configured to calculate the temperature distribution (ΔT) along the deployed fiber using the following equation: Δ v B4 =K ε4 Δε 4 +K T4 ΔT=K T4 ΔT wherein: K T4 is a temperature coefficient of the fourth core; and, wherein there is no fourth bend induced strain distribution (Δε 4 ) associated with the fourth core because the bend applied to the fiber does not cause a change in a length of the fourth core. 5 . The Brillouin-based distributed fiber sensor of claim 2 , wherein the processing system is further configured to calculate the first, second, and third bend induced strain distribution (Δε 1 , Δε 2 , Δε 3 ) using the following equations: Δɛ 1 = 1 K ɛ 1 ( Δ v B 1 - K T 1 K T 4 Δ v B 4 ) ; Δɛ 2 = 1 K ɛ 2 ( Δ v B 2 - K T 2 K T
for measuring angles or tapers; for testing the alignment of axes · CPC title
the material being an optical fibre · CPC title
using changes in transmittance, scattering or luminescence in optical fibres · CPC title
Physics · mapped topic
for measuring radius of curvature {(measuring diameter G01B11/08)} · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.