Fiber Bragg grating-based pressure sensor for a pressure bottle
US-11162852-B1 · Nov 2, 2021 · US
US2023033128A1 · US · A1
| Field | Value |
|---|---|
| Publication number | US-2023033128-A1 |
| Application number | US-202117386871-A |
| Country | US |
| Kind code | A1 |
| Filing date | Jul 28, 2021 |
| Priority date | Jul 28, 2021 |
| Publication date | Feb 2, 2023 |
| Grant date | — |
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An optical system performs a method for measuring an acoustic signal in a wellbore. The optical system includes a light source, an optical fiber and a detector. The light source generates a light pulse. The optical fiber has a first end for receiving the light pulse from the light source and a plurality of enhancement scatterers spaced along a length of the optical fiber for reflecting the light pulse. A longitudinal density of the enhancement scatterers increases with a distance from the first end to increase a signal enhancement generated by the enhancement scatterers distal from the first end. The detector is at the first end of the optical fiber and measures a reflection of the light pulse at the enhancement scatterers to determine the acoustic signal.
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What is claimed is: 1 . An optical system for measuring an acoustic signal in a wellbore, comprising: a light source for generating a light pulse; an optical fiber having a first end for receiving the light pulse from the light source and a plurality of enhancement scatterers spaced along a length of the optical fiber for reflecting the light pulse, wherein a longitudinal density of the enhancement scatterers increases with a distance from the first end to increase a signal enhancement generated by the enhancement scatterers distal from the first end; and a detector at the first end for measuring a reflection of the light pulse at the enhancement scatterers to determine the acoustic signal. 2 . The optical system of claim 1 , wherein the plurality of enhancement scatterer includes a broadband Fiber Bragg grating. 3 . The optical system of claim 2 , wherein the light source is a laser and a reflection bandwidth of the broadband Fiber Bragg grating is greater than a bandwidth of the laser and includes a central wavelength of the laser. 4 . The optical system of claim 1 , wherein the longitudinal density of the scatterers in the optical fiber increases as one of: (i) an exponential function; (ii) an approximately exponential function; (iii) a linear function; and (iv) a non-linear function. 5 . The optical system of claim 1 , wherein a signal enhancement from a gauge length of the optical fiber increases with distance of the gauge length from the light source in relation to a longitudinal density of enhancement scatterers within the gauge length. 6 . The optical system of claim 1 , wherein the light source, optical fiber and detector are used as a Distributed Acoustic Sensing system. 7 . The optical system of claim 1 , wherein the number of enhancement scatterers in the optical fiber is greater than or equal to 100. 8 . The optical system of claim 1 , wherein a first longitudinal density of enhancement scatterers within a first gauge length at a first location near the light source is less than a second longitudinal density of enhancement scatterers within a second gauge length at a second location away from the light source, wherein a signal enhancement from the second gauge length is greater than a signal enhancement from the first gauge length. 9 . A method for obtaining an acoustic measurement in a wellbore, comprising: transmitting a pulse of light from a light source into a first end of an optical fiber, the optical fiber having a plurality of enhancement scatterers spaced along a length of the optical fiber for enhancing the light signal, wherein a longitudinal density of the enhancement scatterers decreases with a distance from the first end to increase a signal enhancement generated by enhancement scatterers distal from the first end; and receiving a reflection of the light pulse from the enhancement scatterers at a detector at the first end to determine the acoustic signal. 10 . The method of claim 9 , wherein the plurality of enhancement scatterer includes a broadband Fiber Bragg grating. 11 . The method of claim 10 , wherein the light source is a laser and a reflection bandwidth of the broadband Fiber Bragg grating is greater than a bandwidth of the laser and includes a central wavelength of the laser. 12 . The method of claim 9 , wherein the light source is a laser and a bandwidth of the enhancement scatterer is greater than a bandwidth of the laser. 13 . The method of claim 9 , wherein the density of the scatterers in the optical fiber decreases as one of: (i) an exponential function; (ii) an approximately exponential function; (iii) a linear function; and (iv) a non-linear function. 14 . The method of claim 9 , wherein a signal enhancement from a gauge length of the optical fiber increases with distance of the gauge length from the light source in relation to a longitudinal density of enhancement scatterers within the gauge length. 15 . The method of claim 9 , wherein a first longitudinal density of enhancement scatterers within a first gauge length at a first location near the light source is less than a second longitudinal density of enhancement scatterers within a second gauge length at a second location away from the light source, wherein a signal enhancement from the second gauge length is greater than a signal enhancement from the first gauge length
characterised by their structure, wavelength response (G02B6/02114, G02B6/02171, G02B6/02195 take precedence; multiple layer cores or claddings G02B6/036, protective coverings G02B6/4429) · CPC title
using elastic backscattering to detect the measured quantity, e.g. using Rayleigh backscattering · CPC title
using a Bragg gratings · CPC title
specially adapted for well-logging · CPC title
using fibre optic sensors (light guides per se G02B6/00, acousto-optical devices specially adapted for gating or modulating in optical wave guides G02F1/125) · CPC title
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