Distributed acoustic sensing system with variable spatial resolution

• US 9,869,795 B2
• Filed: 08/30/2013
• Issued: 01/16/2018
• Est. Priority Date: 08/30/2013
• Status: Active Grant

• Current Assignee: Halliburton Energy Services Incorporated (Halliburton Company)
• Original Assignee: Halliburton Energy Services Incorporated (Halliburton Company)
• Inventors: Jaaskelainen, Mikko
• Primary Examiner(s): Shah, Manish S
• Assistant Examiner(s): Morello, Jean
• Application Number:
  US14/907,790
• Publication Number:
  US 20160170081A1
• Time in Patent Office: 1,600 Days
• Field of Search: 7315258, 356477, 356478
• CPC Class Codes: E21B 47/00 Survey of boreholes or wells monitoring pressure or flow of drilling fluid E21B21/08
• CPC Class Codes: E21B 47/107 using acoustic means
• CPC Class Codes: E21B 47/14 using acoustic waves
• CPC Class Codes: G01V 1/42 using generators in one well and receivers elsewhere or vice versa G01V1/52 takes precedence
• CPC Class Codes: G01V 11/00 Prospecting or detecting by methods combining techniques covered by two or more of main groups G01V1/00 - G01V9/00
• CPC Class Codes: G01V 8/10 Detecting, e.g. by using light barriers by reflection from the object G01S17/00

Abstract

Systems and methods for distributed acoustic sensing based on coherent Rayleigh scattering are disclosed herein. A system comprises a pulse generator, an optical fiber coupled to the pulse generator, an interferometer coupled to the optical fiber, a photodetector assembly coupled to the interferometer, and an information handling system, which activates two optical gain elements so as to vary the optical path length of the interferometer. A method comprises sending an optical pulse down an optical fiber, splitting backscattered light from the optical pulse into a first backscattered pulse and a second backscattered pulse, activating a first optical gain element and a second optical gain element, sending the first backscattered pulse into a first arm of an interferometer, sending the second backscattered pulse into a second arm of an interferometer, combining the first and second backscattered pulses to form an interferometric signal, and receiving the interferometric signal at a photodetector assembly.

Claims

1. A distributed acoustic sensing system based on coherent Rayleigh scattering, comprising:

a pulse generator, which generates an optical pulse;

an optical fiber coupled to the pulse generator;

an interferometer coupled to the optical fiber, further comprising;

a first interferometer arm coupled to a first optical gain element;

a second interferometer arm coupled to a second optical gain element; and

a third interferometer arm coupled to a third optical gain element;

a photodetector assembly coupled to the interferometer, wherein the photodetector assembly detects backscattered interfered light; and

an information handling system, which activates two optical gain elements of the first optical gain element, the second optical gain element, and the third optical gain element so as to vary the optical path length of the interferometer, thereby changing the spatial resolution of the system.

2. The system of claim 1, wherein the first, second, and third interferometer arms have different lengths.

3. The system of claim 1, wherein the interferometer is disposed between the pulse generator and the optical fiber.

4. The system of claim 1, wherein the optical fiber is disposed between the interferometer and the pulse generator.

5. The system of claim 1, wherein the optical fiber is arranged in coils.

6. The system of claim 1, wherein the optical fiber is adapted to be disposed downhole.

7. The system of claim 6, wherein the optical fiber is coupled to at least one of a casing and a tubing.

8. The system of claim 6, wherein the backscattered interfered light is representative of a downhole condition.

9. The system of claim 8, wherein the downhole condition is selected from a group consisting of:

perforations, monitoring downhole pumps and hardware, sensing acoustic signals during fracturing and in-flow stimulation, water injection, production monitoring, flow regimes, reflection seismic, micro-seismic, leaks, cross-flow, and formation compaction.

10. The system of claim 1, wherein the information handling system activates the first and third optical gain elements.

11. The system of claim 1, wherein the information handling system activates the first and second optical gain elements.

12. The system of claim 1, further comprising:

a low reflection device coupled to the optical fiber.

13. The system of claim 1, wherein the pulse generator is operable to generate optical pulses having variable pulse widths.

14. The system of claim 13, wherein a portion of an optical pulse is reflected along the optical fiber according to Rayleigh backscatter.

15. A method for distributed acoustic sensing comprising:

sending a first optical pulse down an optical fiber, wherein light from the first optical pulse is backscattered from positions along the length of the optical fiber according to coherent Rayleigh scattering;

splitting backscattered light from the first optical pulse into a first backscattered pulse and a second backscattered pulse;

activating a first optical gain element and a second optical gain element;

sending the first backscattered pulse into a first arm of an interferometer, the first arm of the interferometer comprising the first optical gain element;

sending the second backscattered pulse into a second arm of an interferometer, the second arm of the interferometer comprising the second optical gain element;

combining the first and second backscattered pulses to form an interferometric signal;

receiving the interferometric signal at a photodetector assembly;

providing output relating to the interferometric signal to an information handling system.

16. The method of claim 15, further comprising:

sending a second optical pulse down the optical fiber; and

varying the activation of the first and second optical gain elements in the interferometer.

17. The method of claim 16, wherein light from the second optical pulse is backscattered from positions along the length of the optical fiber according to coherent Rayleigh scattering;

the method further comprising;

splitting backscattered light from the second optical pulse into a third backscattered pulse and a fourth backscattered pulse; and

wherein varying the activation of the first and second optical gain elements in the interferometer comprises;

activating the first optical gain element and a third optical gain element;

de-activating the second optical gain element;

sending the third backscattered pulse into the first arm of an interferometer;

sending the fourth backscattered pulse into a third arm of an interferometer, the third arm of the interferometer comprising the third optical gain element.

18. A method for distributed acoustic sensing comprising:

generating a first optical pulse;

splitting the first optical pulse into a first portion and a second portion;

activating a first optical gain element and a second optical gain element;

sending the first portion into a first arm of an interferometer, the first arm of the interferometer comprising the first optical gain element;

sending the second portion into a second arm of an interferometer, the second arm of the interferometer comprising the second optical gain element;

combining the first portion from the first arm and second portion from the second arm;

sending the first and second portions down an optical fiber, wherein light from the first and second portions is backscattered from positions along the length of the optical fiber according to coherent Rayleigh scattering to form an interferometric signal;

receiving the interferometric signal at a photodetector assembly;

providing output relating to the interferometric signal to an information handling system.

19. The method of claim 18, further comprising:

generating a second optical pulse; and

varying the activation of the first and second optical gain elements in the interferometer.

20. The method of claim 19, wherein light from the second optical pulse is backscattered from positions along the length of the optical fiber according to coherent Rayleigh scattering;

the method further comprising;

splitting the second optical pulse into a third portion and a fourth portion; and

wherein varying the activation of the first and second optical gain elements in the interferometer comprises;

activating the first optical gain element and a third optical gain element;

de-activating the second optical gain element;

sending the third portion into the first arm of an interferometer;

sending the fourth portion into a third arm of an interferometer, the third arm of the interferometer comprising the third optical gain element.