Method and apparatus for detecting pressure distribution in fluids
View Patent ↗A pressure sensing apparatus has a light source for transmitting pulses of light along a monomode optical fiber. The polarization of light backscattered from the light pulses in the optical fiber is detected by a polarization processing unit (PPU) and a photo detector. The optical fiber is adapted to deform asymmetrically under the influence of applied external isotropic pressure, e.g. from a fluid. The deformation causes the birefringence of the optical fiber to change proportionally to the applied pressure. The change in birefringence can be determined from the detected polarization of the backscattered light, allowing detection of pressure distribution in the fluid. Importantly, the construction of the optical fiber is such that the birefringence beat length of the optical fiber at the wavelength of light propagated by the fiber remains more than twice the spatial length of the light pulses transmitted along the optical fiber. Applications of the invention include detection of fluid flow; location of an interface between two fluids of different density; and tsunami detection.
1. An apparatus for detecting pressure distribution in a fluid, the apparatus comprising:
an optical waveguide for submersion in the fluid, the optical waveguide being adapted to deform asymmetrically transverse to its length on exertion of substantially isotropic pressure by the fluid such that birefringence of the waveguide varies with the exerted pressure;
a light source for directing pulses of light into the waveguide;
a polarisation detector for detecting polarisation states of light backscattered from the light pulses in the waveguide; and
a processor for deriving an indication of the birefringence of at least part of the waveguide from the detected polarisation states to detect pressure distribution in the fluid.
2. The apparatus of claim 1 , wherein the optical waveguide is a side-hole optical fibre.
3. The apparatus of claim 2 , wherein the side-hole fibre has two holes, one on either side of the fibre's core, and the angle subtended by the radius of each hole around the centre of the core is less than around 25°.
4. The apparatus of claim 2 , wherein the side-hole fibre has two holes, one on either side of the fibre's core, and the angle subtended by the radius of each hole around the centre of the core is less than around 10°.
5. The apparatus of claim 1 , wherein the optical waveguide is a D-shaped optical fibre.
6. The apparatus of claim 1 , wherein the polarisation detector is able to detect the polarisation state of light following backscattering at different points along the length of the waveguide and the at least part of the waveguide for which the processor derives an indication of birefringence is between at least some of these points.
7. The apparatus of claim 1 , wherein the processor derives an indication of the variation of birefringence along the length of the waveguide to detect spatial pressure distribution in the fluid.
8. The apparatus of claim 1 , wherein the processor derives an indication of the birefringence of the at least part of the waveguide more than once to detect temporal pressure distribution in the fluid.
9. The apparatus of claim 1 , wherein the optical waveguide is adapted to be placed in a down-hole of an oil well for detecting pressure distribution of fluid in the down-hole.
10. The apparatus of claim 1 , wherein the optical waveguide is adapted to be placed in a water pipe for detecting pressure distribution of water in the pipe.
11. An apparatus for detecting fluid flow, the apparatus comprising: the apparatus of claim 1 wherein the derived indication detects the distribution along the waveguide of the pressure exerted by the fluid on the waveguide; and means for distinguishing a component of the indication resulting from static fluid pressure from a component of the indication resulting from fluid flow.
12. An apparatus for locating an interface between two fluids of different density, the apparatus comprising the apparatus of claim 1 , wherein the optical waveguide is able to extend through the fluids, and means for locating a change in the gradient of the detected pressure distribution along the waveguide to locate the fluid interface.
13. An apparatus for detecting a tsunami, the apparatus comprising the apparatus of claim 1 , wherein the optical waveguide is able to extend underwater along an expected path of the tsunami, the processor derives an indication of the distribution along the waveguide of the pressure exerted by the water on the waveguide and the apparatus has means for determining when changes in the distribution are characteristic of a tsunami travelling through the water along the expected path.
14. The apparatus of claim 1 , comprising more than one waveguide.
15. The apparatus of claim 1 , wherein the optical waveguide extends for several tens of kilometers.
16. The apparatus of claim 1 , wherein the birefringence beat length of the optical waveguide remains more than about 1 m over the range of fluid pressures in which it is intended to use the waveguide.
17. The apparatus of claim 1 , wherein the optical waveguide has intrinsic birefringence beat length longer than around 10 m.
18. The apparatus of claim 1 , wherein the waveguide is arranged such that birefringence induced by increasing fluid pressure opposes (the) intrinsic birefringence of the waveguide.
19. The apparatus of claim 1 , wherein the waveguide has a value of intrinsic birefringence selected such that the waveguide has substantially zero birefringence at a pressure offset from atmospheric pressure to define a range of fluid pressures detectable using the waveguide.
20. The apparatus of claim 1 , wherein the waveguide has deformability selected to control the rate of change of induced birefringence with increasing fluid pressure and thereby to define a/the range of fluid pressures detectable using the waveguide.
21. The apparatus of claim 1 , wherein the waveguide comprises an optical fibre having an elliptical core.
22. The apparatus of claim 1 , wherein the birefringence beat length of the optical waveguide remains above around two times the length of the light pulses over the range of fluid pressures in which it is intended to use the waveguide.
23. An optical waveguide for use in detecting pressure distribution in a fluid, the waveguide being adapted to deform asymmetrically transverse to its length on exertion of substantially isotropic pressure by the fluid such that the birefringence of the waveguide varies with the exerted pressure.
24. The waveguide of claim 23 , wherein the birefringence beat length of the optical waveguide remains more than about 1 m over the range of fluid pressures in which it is intended to use the waveguide.
25. The optical waveguide of claim 23 , having intrinsic birefringence beat length longer than 10 m.
26. The waveguide of claim 23 , arranged such that birefringence induced by increasing fluid pressure opposes (the) intrinsic birefringence of the waveguide.
27. The waveguide of claim 23 , having a value of intrinsic birefringence selected such that the waveguide has substantially zero birefringence at a pressure offset from atmospheric pressure to define a range of fluid pressures detectable using the waveguide.
28. The waveguide of claim 23 , having deformability selected to control the rate of change of induced birefringence with increasing fluid pressure and thereby to define a/the range of fluid pressures detectable using the waveguide.
29. The waveguide of claim 23 , comprising a side-hole optical fibre.
30. The waveguide of claim 23 , comprising an optical fibre having an elliptical core.
31. The waveguide of claim 23 , having birefringence beat length that remains above around two times the length of light pulses used to interrogate the waveguide over the range of fluid pressures in which it is intended to use the waveguide.
32. A method of detecting pressure distribution in a fluid using an optical waveguide for submersion in the fluid, the optical waveguide being adapted to deform asymmetrically transverse to its length on exertion of substantially isotropic pressure by the fluid such that birefringence of the waveguide varies with the exerted pressure, the method comprising:
directing pulses of light into the waveguide;
detecting polarisation states of light backscattered from the light pulses in the waveguide; and
deriving an indication of the birefringence of at least part of the waveguide from the detected polarisation states to detect pressure distribution in the fluid.
33. The method of claim 32 , wherein the optical waveguide is a side-hole optical fibre.
34. The method of claim 33 , wherein the side-hole fibre has two holes, one on either side of the fibre's core, and the angle subtended by the radius of each hole around the centre of the core is less than around 25°.
35. The method of claim 33 , wherein the side-hole fibre has two holes, one on either side of the fibre's core, and the angle subtended by the radius of each hole around the centre of the core is less than around 10°.
36. The method of claim 32 , wherein the optical waveguide is a D-shaped optical fibre.
37. The method of claim 32 , comprising detecting the polarisation state of light following backscattering at different points along the length of the waveguide and wherein the at least part of the waveguide for which the indication of birefringence is determined is between at least some of these points.
38. The method of claim 32 , comprising deriving an indication of the variation of birefringence along the length of the waveguide to detect spatial pressure distribution in the fluid.
39. The method of claim 32 , comprising deriving an indication of the birefringence of the at least part of the waveguide more than once to detect temporal pressure distribution in the fluid.
40. The method of claim 32 , wherein the optical waveguide is placed in a down-hole of an oil well and the pressure distribution of fluid in the down-hole is detected.
41. The method of claim 32 , wherein the optical waveguide is placed in a water pipe and the pressure distribution of water in the water pipe is detected.
42. A method of detecting fluid flow, the method comprising: using the method of claim 32 , wherein the derived indication detects the distribution along the waveguide of the pressure exerted by the fluid on the waveguide; and distinguishing a component of the indication resulting from static fluid pressure from a component of the indication resulting from fluid flow.
43. A method of locating an interface between two fluids of different density, the method comprising the method of claim 32 , wherein the optical waveguide extends through the fluids, and locating a change in the gradient of the detected pressure distribution along the waveguide to locate the fluid interface.
44. A method of detecting a tsunami, the method comprising the method of claim 32 , wherein the optical waveguide extends underwater along an expected path of a tsunami, the derived indication is of the distribution along the waveguide of the pressure exerted by the water on the waveguide, and determining when changes in the distribution are characteristic of a tsunami travelling through the water along the expected path.
45. The method of claim 32 , comprising more than one waveguide.
46. The method of claim 32 , wherein the optical waveguide extends for several tens of kilometers.
47. The method of claim 32 , wherein the birefringence beat length of the optical waveguide remains more than about 1 m over the range of fluid pressures in which it is intended to use the waveguide.
48. The method of claim 32 , wherein the optical waveguide has intrinsic birefringence beat length longer than around 10 m.
49. The method of claim 32 , wherein the waveguide is arranged such that birefringence induced by increasing fluid pressure opposes (the) intrinsic birefringence of the waveguide.
50. The method of claim 32 , comprising selecting a value of intrinsic birefringence such that the waveguide has substantially zero birefringence at a pressure offset from atmospheric pressure to define a range of fluid pressures detectable using the waveguide.
51. The method of claim 32 , comprising selecting the deformability of the waveguide to control the rate of change of induced birefringence with increasing fluid pressure and thereby to define a/the range of fluid pressures detectable using the waveguide.
52. The method of claim 32 , comprising an optical fibre having an elliptical core.
53. The method of claim 32 , wherein the birefringence beat length of the optical waveguide remains above around two times the length of (the) light pulses (used to interrogate the waveguide) over the range of fluid pressures in which it is intended to use the waveguide.
54. A non-transitory computer readable medium comprising a program code adapted to carry out the method of claim 32 when processed by a processing means.
55. A method of detecting pressure distribution in a fluid using a waveguide adapted to deform asymmetrically transverse to its length on exertion of substantially isotropic pressure by the fluid such that the birefringence of the waveguide varies with exerted pressure.
56. The method of claim 55 , wherein the birefringence beat length of the optical waveguide remains more than 1 m over the range of fluid pressures in which it is intended to use the waveguide.
57. The method of claim 55 , wherein the optical waveguide has intrinsic birefringence beat length longer than around 10 m.
58. The method of claim 55 , wherein the waveguide is arranged such that birefringence induced by increasing fluid pressure opposes (the) intrinsic birefringence of the waveguide.
59. The method of claim 55 , comprising selecting a value of intrinsic birefringence such that the waveguide has substantially zero birefringence at a pressure offset from atmospheric pressure to define a range of fluid pressures detectable using the waveguide.
60. The method of claim 55 , comprising selecting the deformability of the waveguide to control the rate of change of induced birefringence with increasing fluid pressure and thereby to define a/the range of fluid pressures detectable using the waveguide.
61. The method of claim 55 , comprising an optical fibre having an elliptical core.
62. The method of claim 55 , wherein the birefringence beat length of the optical waveguide remains above around two times the length of (the) light pulses (used to interrogate the waveguide) over the range of fluid pressures in which it is intended to use the waveguide.