Downhole referencing techniques in borehole surveying

• US 6,882,937 B2
• Filed: 02/18/2003
• Issued: 04/19/2005
• Est. Priority Date: 02/18/2003
• Status: Expired due to Fees

• Current Assignee: Schlumberger Technology Corporation (Schlumberger NV)
• Original Assignee: Pathfinder Energy Services LLC (Schlumberger NV)
• Inventors: McElhinney, Graham
• Primary Examiner(s): MCELHENY JR, DONALD E
• Application Number:
  US10/369,353
• Publication Number:
  US 20040163443A1
• Time in Patent Office: 791 Days
• Field of Search: 702/6, 702/9, 702/10, 333/04, 333/13
• US Class Current: 702/9
• CPC Class Codes: E21B 47/022 of the borehole, e.g. using geomagnetism

Abstract

A method for determining rotational offset between first and second gravity measurement devices deployed on a downhole tool is disclosed. The method includes positioning the tool in a previously surveyed section of a borehole that provides a historical survey including at least three previously surveyed azimuthal reference points and utilizing the gravity measurement devices to determine local azimuths at three or more sites in the previously surveyed section of the borehole. The method further includes comparing local azimuths with the historical survey and determining a rotational offset between the measurement devices that gives a best fit between local azimuths and the historical survey. A system adapted to execute the disclosed method and a computer system including computer-readable logic configured to instruct a processor to execute the disclosed method are also provided.

Claims

1. A method for determining rotational offset between first and second gravity measurement devices, the first and second gravity measurement devices disposed at corresponding first and second positions on a downhole tool deployed in a borehole, the method comprising:

(a) positioning the tool in a previously surveyed section of borehole, the previously surveyed section providing a historical survey including at least three previously surveyed azimuthal reference points within the previously surveyed section of borehole;

(b) determining local azimuths at three or more sites in the previously surveyed section of the borehole using the first and second gravity measurement devices;

(c) comparing local azimuths determined in (b) with the historical survey; and

(d) determining a rotational offset between the first and second measurement devices that gives a best fit in (c) between local azimuths determined in (b) and the historic survey.

2. The method of claim 1, wherein (a) comprises co-locating one of the first and second gravity measurement devices at a predetermined one of the previously surveyed azimuthal reference points.

3. The method of claim 2, wherein at least one local azimuth determined in (b) is referenced to the predetermined previously surveyed azimuth reference point.

4. The method of claim 3, wherein further local azimuths determined in (b) are chain referenced to the predetermined previously surveyed azimuthal reference point.

5. The method of claim 1, wherein (b) comprises utilizing the first and second gravity measurement devices to determine local azimuths at five or more sites in the previously surveyed section of the borehole.

6. The method of claim 5, wherein at least five of said five or more local azimuths are chain referenced to a predetermined one of the previously surveyed azimuthal reference points.

7. The method of claim 1, wherein (b) comprises:

measuring first and second gravity vector sets at each of the three or more sites; and

determining the local azimuths at the three or more sites using the gravity vector sets.

8. The method of claim 7, wherein the gravity vector sets each comprise first and second gravity vectors.

9. The method of claim 8, wherein (b) further comprises deriving a third gravity vector for each of the gravity vector sets, each third gravity vector derived from processing the corresponding first and second gravity vectors and a known total gravitational field of the Earth.

10. The method of claim 7, wherein the gravity vector sets each comprise first, second, and third gravity vectors.

11. The method of claim 7, wherein:

each of the local azimuths determined in (b) is determined by adding a change in borehole azimuth between the first and second gravity measurement devices to a reference borehole azimuth; and

the gravity vector sets are utilized to determine the change in borehole azimuth.

12. The method of claim 11, wherein the change in borehole azimuth is determined according to the equation:

$\begin{array}{c}\mathrm{DeltaAzi}=\frac{\mathrm{Beta}}{1-\mathrm{Sin}<br><br>\left(\left(\mathrm{Inc1}+\mathrm{Inc2}\right)/2\right)}\\ \mathrm{wherein}\\ \mathrm{Beta}=\arctan <br><br>\left(\frac{\begin{array}{c}\left(\mathrm{Gx2}*\mathrm{Gy1}-\mathrm{Gy2}*\mathrm{Gx1}\right)*\\ \sqrt{{\mathrm{Gx1}}^2+{\mathrm{Gy1}}^2+{\mathrm{Gz1}}^2}\end{array}}{\begin{array}{c}(\mathrm{Gz2}*\left({\mathrm{Gx1}}^2+{\mathrm{Gy1}}^2\right)+\\ \mathrm{Gz1}*\left(\mathrm{Gx2}*\mathrm{Gx1}+\mathrm{Gy2}*\mathrm{Gy1}\right)\end{array}}\right);<br><br>\\ \mathrm{Inc1}=\arctan \left(\frac{\sqrt{({\mathrm{Gx1}}^2+{\mathrm{Gy1}}^2}}{\mathrm{Gz1}}\right);<br><br>\\ \mathrm{Inc2}=\arctan \left(\frac{\sqrt{({\mathrm{Gx2}}^2+{\mathrm{Gy2}}^2}}{\mathrm{Gz2}}\right);<br><br>\mathrm{and}\end{array}$

wherein DeltaAzi represents the change in borehole azimuth, Gx1, Gy1, and Gz1, represent first, second, and third gravity vectors measured with the first gravity measurement device and Gx2, Gy2, and Gz2, represent first, second, and third gravity vectors measured with the second gravity measurement device.

13. The method of claim 11, wherein the reference borehole azimuth is determined utilizing a supplemental reference measurement device.

14. The method of claim 13, wherein the supplemental reference measurement device comprises a gyroscope disposed at one of the first and second positions on the downhole tool.

15. The method of claim 1, wherein (b) further comprises determining local azimuths for a plurality of projected rotational offset values.

16. The method of claim 1, wherein said comparing in (c) comprises plotting local azimuths and the previously surveyed azimuthal reference points verses a borehole depth at a plurality of projected rotational offsets.

17. The method of claim 1, wherein said comparing in (c) comprises generating a plan view of local azimuths and the previously surveyed azimuthal reference points at a plurality of projected rotational offsets.

18. The method of claim 1, wherein said determining in (d) comprises utilizing numerical methods to determine a rotational offset at which the local azimuths give said best fit to the historical survey.

19. The method of claim 1, wherein (b) further comprises:

measuring first and second gravity vector sets at each of the three or more sites;

determining corrected gravity vector set at each of the three or more sites using a projected rotational offset;

replacing one of the gravity vector sets at each of the three or more sites with the corresponding corrected gravity vector set; and

determining the local azimuths at each of the three or more sites using the corrected gravity vector sets.

20. The method of claim 19, wherein the corrected gravity vector set is determined according the equations:

$\begin{array}{c}\mathrm{Gxcorrected}=\sin <br><br>\left(\arctan <br><br>\left(\frac{\mathrm{Gx}}{\mathrm{Gy}}\right)+\mathrm{Rc}\right)<br><br>\sqrt{({\mathrm{Gx}}^2+{\mathrm{Gy}}^2}\\ \mathrm{Gycorrected}=\cos <br><br>\left(\arctan <br><br>\left(\frac{\mathrm{Gx}}{\mathrm{Gy}}\right)+\mathrm{Rc}\right)<br><br>\sqrt{({\mathrm{Gx}}^2+{\mathrm{Gy}}^2}\\ \mathrm{Gzcorrected}=\mathrm{Gz}\end{array}$

wherein Gxcorrected, Gycorrected, and Gzcorrected represent corrected gravity vectors in the corrected gravity vector set, Gx, Gy, and Gz represent gravity vectors in the one of the gravity vector sets, and Rc represents the rotational offset between the first and second gravity measurement devices.

21. The method of claim 1, wherein the previously surveyed section of the borehole has an inclination ranging from about 1 to about 10 degrees.

22. The method of claim 1, wherein the downhole tool comprises a measurement while drilling tool.

23. The method of claim 1, wherein the downhole tool is coupled to a drill string.

24. A method for determining rotational offset between first and second gravity measurement devices, the first and second gravity measurement devices disposed at corresponding first and second positions on a downhole tool deployed in a borehole, the method comprising:

(a) positioning the tool in a previously surveyed section of borehole the previously surveyed section providing a historical survey including at least three previously surveyed azimuthal reference points within the previously surveyed section of the borehole;

(b) measuring first and second gravity vector sets using the first and second gravity measurement devices at each of five or more sites;

(c) determining a set of corrected gravity vectors at each of the five or more sites using a projected rotational offset;

(d) replacing one of the gravity vector sets at each of the five or more sites with the corresponding corrected gravity vector set determined in (c);

(e) determining the local azimuths at each of the five or more sites using the corrected gravity vector sets;

(f) comparing the local azimuths determined in (e) with the historical survey;

(g) determining a rotational offset between the first and second measurement devices that gives a best fit in (f) between local azimuths determined in (e) and the historical survey.

25. A method for determining rotational offset between first and second gravity measurement devices, the first and second gravity measurement devices disposed at corresponding first and second positions on a downhole tool deployed in a borehole, the method comprising:

(a) positioning the tool in a previously surveyed section of borehole, the previously surveyed section providing a historical survey including at least three previously surveyed azimuthal reference points within the previously surveyed section of borehole;

(b) measuring first and second gravity vector sets using the first and second gravity measurement devices;

(c) determining local azimuths using the gravity vector sets measured in (b);

(d) repeating (b) and (c) at two or more additional sites in the previously eyed section of the borehole;

(e) comparing the local azimuths determined in (c) and (d) with the historical survey; and

(f) determining a rotational offset between the first and second measurement devices that gives a best fit in (e) between local azimuths determined in (c) and (d) and the historical survey.

26. A system for determining rotational offset between first and second gravity measurement devices deployed in a borehole, the system comprising:

a down hole tool including first and second gravity measurement devices deployed thereon, the tool operable to be positioned in a previously surveyed section of borehole, the previously surveyed section providing a historical survey including at least three previously surveyed azimuthal reference points within the previously surveyed section of borehole; and

a processor configured to determine;

(A) local azimuths at three or more sites in the previously surveyed section of the borehole from readings taken from the first and second gravity measurement devices;

(B) a comparison of local azimuths determined in (A) with the historical survey; and

(C) a rotational offset between the first and second measurement devices that gives a best fit in (B) between local azimuths determined in (A) and the historical survey.

27. The system of claim 26, wherein:

each of the gravity measurement devices comprises first, second, and third accelerometers.

28. A computer system comprising:

at least one processor; and

a storage device having computer-readable logic stored therein, the computer-readable logic accessible by and intelligible to the processor;

the processor further disposed to receive input from first and second gravity measurement devices when said first and second measurement devices are deployed at corresponding first and second positions in a borehole, the first and second positions located within a previously surveyed section of borehole;

the processor further having access to a historical survey of the previously surveyed section of borehole, the historical survey including at least three previously surveyed azimuthal reference points within the previously surveyed section of borehole;

the computer-readable logic further configured to instruct the processor to execute a method for determining rotational offset between the first and second gravity measurement devices, the method comprising;

(a) determining local azimuths at three or more sites in the previously surveyed section of borehole using input from the first and second gravity measurement devices;

(b) comparing local azimuths determined in (a) with the historical survey; and

(c) determining a rotational offset between the first and second measurement devices that gives a best fit in (b) between local azimuths determined in (a) and the historical survey.

29. The computer system of claim 28, wherein:

the local azimuths are determined in (a) by adding a change in borehole azimuth between the first and second gravity measurement devices to a reference borehole azimuth; and

the change in borehole azimuth is determined according to the equation;

$\begin{array}{c}\mathrm{DeltaAzi}=\frac{\mathrm{Beta}}{1-\mathrm{Sin}<br><br>\left(\left(\mathrm{Inc1}+\mathrm{Inc2}\right)/2\right)}\\ \mathrm{wherein}\\ \mathrm{Beta}=\mathrm{arc}<br><br>\text{\hspace{1em}<br><br>}<br><br>\tan <br><br>\left(\frac{\begin{array}{c}\left(\mathrm{Gx2}*\mathrm{Gy1}-\mathrm{Gy2}*\mathrm{Gx1}\right)*\\ \sqrt{{\mathrm{Gx1}}^2+{\mathrm{Gy1}}^2+{\mathrm{Gz1}}^2}\end{array}}{\begin{array}{c}\mathrm{Gz2}*\left({\mathrm{Gx1}}^2+{\mathrm{Gy1}}^2\right)+\mathrm{Gz1}*\\ \left(\mathrm{Gx2}*\mathrm{Gx1}+\mathrm{Gy2}*\mathrm{Gy1}\right)\end{array}}\right);<br><br>\\ \mathrm{Inc1}=\mathrm{arc}<br><br>\text{\hspace{1em}<br><br>}<br><br>\tan \left(\frac{\sqrt{({\mathrm{Gx1}}^2+{\mathrm{Gy1}}^2}}{\mathrm{Gz1}}\right);<br><br>\\ \mathrm{Inc2}=\mathrm{arc}<br><br>\text{\hspace{1em}<br><br>}<br><br>\tan \left(\frac{\sqrt{({\mathrm{Gx2}}^2+{\mathrm{Gy2}}^2}}{\mathrm{Gz2}}\right);<br><br>\mathrm{and}\end{array}$

wherein DeltaAzi represents the change in borehole azimuth, Gx1, Gy1, and Gz1, represent first, second, and third gravity vectors input from the first gravity measurement device and Gx2, Gy2, and Gz2, represent first, second, and third gravity vectors input from the second gravity measurement device.

30. The computer system of claim 28, wherein:

said input from the first and second gravity measurement devices includes corresponding first and second gravity vector sets at each of the three or more sites;

a projected rotational offset is utilized to determine a corrected gravity vector set at each of the three or more sites; and

the corrected gravity vector set is determined according the equations;

$\begin{array}{c}\mathrm{Gxcorrected}=\sin <br><br>\left(\mathrm{arc}<br><br>\text{\hspace{1em}<br><br>}<br><br>\tan <br><br>\left(\frac{\mathrm{Gx}}{\mathrm{Gy}}\right)+\mathrm{Rc}\right)<br><br>\sqrt{({\mathrm{Gx}}^2+{\mathrm{Gy}}^2};<br><br>\\ \mathrm{Gycorrected}=\cos <br><br>\left(\mathrm{arc}<br><br>\text{\hspace{1em}<br><br>}<br><br>\tan <br><br>\left(\frac{\mathrm{Gx}}{\mathrm{Gy}}\right)+\mathrm{Rc}\right)<br><br>\sqrt{({\mathrm{Gx}}^2+{\mathrm{Gy}}^2};<br><br>\end{array}$$\mathrm{Gzcorrected}=\mathrm{Gz};<br><br>$

wherein Gxcorrected, Gycorrected, and Gzcorrected represent corrected gravity vectors in the corrected gravity vector set, Gx, Gy, and Gz represent gravity vectors in the one of the gravity vector sets, and Rc represents the rotational offset between the first and second gravity measurement devices.