Distributed acoustic monitoring is becoming an important method for downhole monitoring of wells, with many potential applications. This technology involves the use of an optical cable having an optical fiber contained within a metal tube, with gels or other substances used to hold the fiber within the tube. As the cable is deformed, the length of the optical fiber is changed, which can be detected through proper optical interrogation of the fiber. Generally, this involves sending short bursts of light down the fiber, and recording the light that is reflected back via Rayleigh backscatter.
In general, in these applications, either incident acoustic pressure or alternatively, the vibration of a surface to which the optical cable is attached, results in the bending of the optical cable. Since the cable is predominately sensitive to longitudinal deformation, care must be taken to ensure that the bending of the cable actually produces a change in the length of the optical fiber. Attempts to increase the sensitivity of the fiber have placed the fiber away from the center of the cable, and nearer to the outside of the cable, as this increases the strain that occurs in the fiber. However, for some applications, such as vertical seismic profiling (“VSP”), even greater sensitivity of the fiber may be needed.
Thus, the art would be receptive to alternative devices and methods for improving the sensitivity of optical fibers in optical cables.
An optical cable includes an outer tubing; at least one optical fiber disposed within the outer tubing; and, a stiffening member configured to bend with bending of the outer tubing; wherein the stiffening member shifts a neutral plane of the cable away from the at least one optical fiber.
An optical cable includes an outer tubing having a central axis, a stiffness of the outer tubing asymmetric with respect to the central axis; and, at least one optical fiber disposed within the outer tubing; wherein a distance between the at least one optical fiber and a neutral plane of the cable is greater than a distance between the at least one optical fiber and the central axis.
A method of increasing a bending sensitivity in an optical cable, the method includes shifting a neutral plane of the cable away from an optical fiber in the cable.
Referring now to the drawings wherein like elements are numbered alike in the several Figures:
One exemplary embodiment of a system 10 for downhole sensing is shown in
The cable 12 includes an outer tubing 16 (cable shell), at least one optical fiber 18 retained in place within the outer tubing 16 with gel or other holding substance 20 (
The system 10 including the cable 12 described herein is usable as a distributed fiber optic sensor or distributed acoustic sensor (“DAS”). The system 10 includes a light source 26 such as a laser, and light from the light source 26 is transferred for propagation along the fiber optic cable 12. Any optical radiation which is Rayleigh back-scattered within the optical fiber 18 is detected by photodetector 28. Any incident acoustic signal causes mechanical vibration of the fiber 18 which changes the amount of Rayleigh back-scattering at that part of the fiber 18. The variation in back-scatter is related to the movement of the fiber 18 and the amount of bending experienced by the fiber 18. The signal from the photodetector 28 is processed by a signal processor 30 and receivable by a user interface (not shown). The light source 26, photodetector 28, and signal processor 30 may be positioned at a surface location.
In an exemplary embodiment shown in
In the mechanics of beams and other members subjected to bending (such as the optical cable 12), the longitudinal elements within the cable 12 are subjected to uniaxial stresses. These stresses are increased the further away from the neutral plane 40 an element is. Increased sensitivity is obtained by placing the fiber 18 further away from the neutral plane 40 of the cable 12, and thus the fiber 18 is located at the inner periphery 36 of the tubing 16. The stresses experienced by the fiber 18 are governed by the equation:
σ=My/I
where σ represents the uniaxial stress applied to the element (fiber 18), M represents the applied bending moment, y represents the distance of the element (fiber 18) from the neutral plane of the cable 12, and I represents the area moment of inertia of the cable. 12 Strain (ε=ΔL/L0, where ΔL is the change in length and L0 is the original length) is a measure of how much an object is being stretched. Strain is caused by stress, and for the material of the fiber 18, stress and strain are linearly related.
While placement of the fiber 18 at the inner periphery 36 distances the fiber 18 from the neutral plane 40, the embodiments of a cable 12 having improved sensitivity to bending further distances the neutral plane from the fiber by moving the neutral plane of the cable 12 away from the fiber 18. This is accomplished by arraying the stiffness of the cable 12 asymmetrically with respect to the central axis 24 of the cable 12, such as by securing a longitudinal stiffening member 22 on a side of the cable 12 opposite the fiber 18. With the fiber 18 positioned at an outermost radial location along the inner periphery 36 of the tubing 16, the stiffening member 22 is disposed on a diametrically opposite side of the inner periphery 36 from the fiber 18. The addition of the stiffening member 22 to the cable 12 serves to move the neutral plane 42 of the cable 12 toward the stiffening member 22. The distance (y) of the optical fiber 18 from the neutral plane 42 of the cable 12 is increased, as compared to the distance of the optical fiber 18 from the neutral plane 40, thereby increasing the longitudinal stress (σ) applied to the optical fiber 18. This increased stress results in increased strain, and correspondingly, increased optical signal.
In
In
In
With respect to the above equation for stress (σ), it is noted that the distance (y) of the fiber 18 from the neutral plane 42 is proportional to the stress (σ), but the area moment of inertia (I) is inversely proportional to the stress (σ). It should be further noted that while increasing the distance (y) of the fiber 18 from the neutral plane 42 of the cable 12, the addition of such a stiffening member 22 on one side of the cable 12 also has the effect of increasing the area moment of inertia of the cable 12 (I), which could result in decreased stress (σ) applied to the fiber 18, and correspondingly decreased signal should the area moment of inertia (I) be too great. Mechanical analysis of such designs reveal that as the area corresponding to the stiffening member 22 increases, initially the former effect (the increase in distance from the neutral plane 42) dominates. However, as the area continues to increase, and the area corresponding to the stiffening member 22 grows closer and closer to the geometric center 32 of the cable 12, the later effect begins to dominate, and the stress applied to the optical fiber 18 decreases. As a result, the size of the stiffening element 22 must be controlled so as to maximize the increase in the applied stress.
While the above-described embodiments have been described with respect to a single fiber 18 within the cable 12, it should be understood that the cable 12 may also include two or more fibers 18 within the cable 12. In order to increase the bending sensitivity of all of the fibers 18 within the cable 12, the arrangement of the fibers 18 should be diametrically opposite the position of the stiffening member 22 to shift the neutral plane 42 away from the fibers 18.
While the invention has been described with reference to an exemplary embodiment or embodiments, it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted for elements thereof without departing from the scope of the invention. In addition, many modifications may be made to adapt a particular situation or material to the teachings of the invention without departing from the essential scope thereof. Therefore, it is intended that the invention not be limited to the particular embodiment disclosed as the best mode contemplated for carrying out this invention, but that the invention will include all embodiments falling within the scope of the claims. Also, in the drawings and the description, there have been disclosed exemplary embodiments of the invention and, although specific terms may have been employed, they are unless otherwise stated used in a generic and descriptive sense only and not for purposes of limitation, the scope of the invention therefore not being so limited. Moreover, the use of the terms first, second, etc. do not denote any order or importance, but rather the terms first, second, etc. are used to distinguish one element from another. Furthermore, the use of the terms a, an, etc. do not denote a limitation of quantity, but rather denote the presence of at least one of the referenced item.
Number | Name | Date | Kind |
---|---|---|---|
4836639 | Shamoto et al. | Jun 1989 | A |
4859025 | Houghton | Aug 1989 | A |
5082380 | Sutehall et al. | Jan 1992 | A |
6137936 | Fitz et al. | Oct 2000 | A |
6459837 | Fitz et al. | Oct 2002 | B1 |
6516124 | Po | Feb 2003 | B2 |
7412135 | Seifert et al. | Aug 2008 | B2 |
7706640 | Pizzorno et al. | Apr 2010 | B2 |
8346040 | Testu et al. | Jan 2013 | B2 |
8676012 | Bradley et al. | Mar 2014 | B2 |
20040112595 | Bostick, III et al. | Jun 2004 | A1 |
20120007717 | De Jong | Jan 2012 | A1 |
20120222487 | Hill et al. | Sep 2012 | A1 |
20120328253 | Hurley et al. | Dec 2012 | A1 |
20130094798 | Duncan et al. | Apr 2013 | A1 |
Number | Date | Country |
---|---|---|
8160265 | Jun 1996 | JP |
2013092036 | May 2013 | JP |
Entry |
---|
D. Miller, et al. (Silixa Ltd.), “Vertical Seismic Profiling Using a Fibre-optic Cable as a Distributed Acoustic Sensor”,74th EAGE Conference & Exhibition incorporating SPE EUROPEC 2012, Copenhagen, Denmark, Jun. 4-7, 2012, pp. 1-5. |
Weatherford International Ltd., “Downhole Optical Cable” Production Optimization, Houston, Texas, www.weatherford.com, 2005-2008 Weatherford, pp. 1-3. |
International Search Report and Written Opinion of PCT Application No. PCT/US2014/050633, dated Nov. 21, 2014, pp. 1-12. |
Number | Date | Country | |
---|---|---|---|
20150083904 A1 | Mar 2015 | US |