Gravity and differential gravity sensor, and system and method for monitoring reservoirs using same

• US 6,671,057 B2
• Filed: 10/31/2001
• Issued: 12/30/2003
• Est. Priority Date: 10/31/2001
• Status: Expired due to Term

• Current Assignee: Schlumberger Technology Corporation (SLB)
• Original Assignee: Schlumberger Technology Corporation (SLB)
• Inventors: Orban, Andre E.
• Primary Examiner(s): Font, Frank G.
• Assistant Examiner(s): CONNOLLY, PATRICK J
• Application Number:
  US09/999,792
• Publication Number:
  US 20030081218A1
• Time in Patent Office: 790 Days
• Field of Search: 356/495, 356/28.5, 733/82.R, 733/82.G, 731/525.4, 731/524.3, 731/524.6
• US Class Current: 356/496
• CPC Class Codes: G01B 9/02097 Self-interferometers
• CPC Class Codes: G01V 7/14 using free-fall time

Abstract

A gravity sensor is disclosed which includes a first mass adapted to free fall when selectively released from an initial position. The mass has optical elements adapted to change a length of an optical path in response to movement of the mass. The sensor output is coupled to a beam splitter. One output of the splitter is coupled substantially optically directly to an interferometer. Another output of the splitter is coupled to the interferometer through an optical delay line. A frequency of the interference pattern is directly related to gravity at the mass. A second such mass having similar optics, optically coupled in series to the first mass and adapted to change the path length in opposed sign, when selectively dropped to cause time coincident movement of the two masses, generates an interference pattern having frequency related to gravity difference.

Claims

1. A gravity difference sensor, comprising:

a first mass adapted to free fall when selectively released, the first mass having optical elements thereon adapted to change a length of an optical path through the sensor in response to movement of the first mass;

a second mass adapted to free fall when selectively released, the second mass having optical elements thereon coupled in optical series with the optical elements on the first mass, the optical elements on the second mass adapted to change a length of the optical path through the sensor in response to movement of the second mass in a sense opposite to the change in length effected by movement of the first mass; and

a beam splitter operatively coupled to an output of the optical path traversed by the sensor, one output of the splitter coupled substantially optically directly to an interferometer, another output of the splitter coupled to the interferometer through an optical delay line.

2. The gravity difference sensor as defined in claim 1 wherein the first mass and the second mass are disposed in a same housing at spaced apart positions.

3. The gravity difference sensor as defined in claim 1 wherein the optical elements on the first mass and the second mass comprise reflectors.

4. The gravity difference sensor as defined in claim 1 further comprising a drop controller adapted to time selective dropping of the first mass and the second mass so that there is at least partially time coincident movement of the first mass and the second mass.

5. The gravity difference sensor as defined in claim 1 wherein the optical elements on the first mass and the second mass comprise optical path splitters adapted to cause a light beam passing through the optical elements to traverse a distance between the optical elements and an optical target a plurality of times, whereby a the change in length of the optical path effected by movement of the first mass and the second mass is a multiple of a change in distance between the first mass and the second mass and the optical target.

6. The gravity difference sensor as defined in claim 1 wherein the optical delay line comprises a selected length of optical fiber.

7. The gravity difference sensor as defined in claim 1 wherein the optical delay line provides a time delay at most equal to an expected fall time of at least one of the first mass and the second mass.

8. The gravity difference sensor as defined in claim 1 further comprising a plurality of masses each adapted to free fall when selectively released, the plurality of masses each having optical elements thereon coupled in optical series with the optical elements on the first mass and the second mass, the optical elements on the plurality of masses adapted to change a length of the optical path through the sensor in response to movement of each of the plurality of masses, each such change in length for each one of the plurality of masses being in a sense opposite to the change in length effected by movement of a one of the plurality of masses in optical series before and after each one of the plurality of masses.

9. The gravity difference sensor as defined in claim 8 further comprising a drop controller adapted to selectively drop the first mass, the second mass and each of the plurality of masses, the drop controller adapted to time the selective dropping of each of the masses so that there is at least partially time coincident movement of each pair of masses adjacent to each other in optical series.

10. The gravity difference sensor as defined in claim 1 further comprising optical elements disposed on the first mass adapted to change the length of the optical path a multiple of a movement distance of the first mass within the sensor.

11. A method for measuring gravity difference, comprising:

illuminating optical elements on a first mass adapted to free fall when released, the optical elements adapted to change a length of an optical path in response to movement of the first mass;

serially illuminating optical elements on a second mass adapted to free fall when released, the optical elements adapted to change a length of an optical path in response to movement of the second mass, the change in length effected by movement of the second mass having a sense opposite to the change in length effected by the first mass;

dropping the first mass at a selected time;

dropping the second mass at a selected time, the dropping the second mass timed to provide at least some time coincident movement of the first mass and the second mass;

splitting light traveling away from the optical elements;

conducting one output of the splitting substantially directly to one input of an interferometer;

conducting another output of the splitting to the interferometer through a selected time delay; and

determining a frequency of an interference pattern in the interferometer during the at least partially time coincident movement, the frequency related to gravity difference between a position of the first mass and a position of the second mass.

12. The method as defined in claim 11 further comprising:

prior to the splitting, directing light leaving the optical elements on the second mass to optical elements on each of a plurality of masses each adapted to free fall when selectively released from an initial position, the optical elements on each of the plurality of masses connected in optical series and adapted to change the length of the optical path in response to the dropping of each of the plurality of masses, the change in length caused by each of the plurality of masses having a sense opposite to the change in length of the previous one of the plurality of masses in the optical series;

selectively dropping each one of the plurality of masses, the selective dropping timed to provide at least partially time-coincident movement of pairs of series-adjacent ones of the plurality of masses; and

determining a frequency of an interference pattern in the interferometer in response to the time-coincident movement of the pairs series-adjacent ones of the plurality of masses, the frequency thereof corresponding to a difference in gravity between positions of each mass in each of the pairs of series-adjacent ones of the plurality of masses.

13. The method as defined in claim 11 further comprising causing light to traverse a path between the first mass and an optical target a plurality of times so that the change in length of the optical path is a multiple of a movement distance of the first mass.

14. A well logging instrument, comprising:

a chassis adapted to be lowered into a wellbore;

a first sensor disposed on the chassis, the first sensor comprising a first mass adapted to free fall when selectively released, the first mass having optical elements thereon adapted to change a length of an optical path through the sensor in response to movement of the first mass;

a second sensor disposed on the chassis at a position spaced apart from the first sensor, the second sensor having a second mass adapted to free fall when selectively released, the second mass having optical elements thereon coupled in optical series with the optical elements on the first mass, the optical elements on the second mass adapted to change a length of the optical path through the sensor in response to movement of the second mass in a sense opposite to the change in length effected by movement of the first mass; and

a beam splitter operatively coupled to an output of the optical path traversed by the sensor, one output of the splitter coupled substantially optically directly to an interferometer, another output of The splitter coupled to the interferometer through an optical delay line.

15. The well logging instrument as defined in claim 14 further comprising a drop controller adapted to time selective release of the first mass and the second mass so that there is at least partially time coincident movement of the first mass and the second mass.

16. The well logging instrument as defined in claim 14 wherein the chassis is adapted to be conveyed into a wellbore at one end of an armored electrical cable.

17. The well logging instrument as defined in claim 16 further comprising a light source disposed at the earth'"'"'s surface, the light source optically coupled to the first sensor by an optical fiber disposed in the well logging cable.

18. The well logging instrument as defined in claim 14 further comprising a plurality of sensor disposed on the chassis at spaced apart positions, each sensor having a mass adapted to free fall when selectively released, the masses each having optical elements thereon coupled in optical series with the optical elements on the first mass and the second mass, the optical elements on the plurality of masses adapted to change a length of the optical path through each sensor in response to movement of each of the plurality of masses, each such change in length for each one of the plurality of masses being in a sense opposite to the change in length effected by movement of a one of the plurality of masses in optical series before and after each one of the plurality of masses.

19. The well logging instrument as defined in claim 18 further comprising a drop controller adapted to selectively drop the first mass, the second mass and each of the plurality of masses, the drop controller adapted to time the selective dropping of each of the masses so that there is at least partially time coincident movement between each pair of masses adjacent to each other in optical series.

20. The well logging instrument as defined in claim 14 further comprising a gravity orientation sensor coupled to the chassis, the orientation sensor adapted to generate a signal corresponding to a direction of earth'"'"'s gravity with respect to the chassis.

21. The well logging instrument as defined in claim 20 wherein the first sensor and the second sensor are each mounted to the chassis in a moveable framework.

22. The well logging instrument as defined in claim 14 further comprising optical elements disposed on the first mass and adapted to the change length of the optical path a multiple of a movement distance of the first mass within the first sensor.

23. The well logging instrument as defined in claim 14 further comprising optical elements disposed on the second mass and adapted to the change length of the optical path a multiple of a movement distance of the second mass within the second sensor.

24. A method for well logging, comprising:

(a) inserting a well logging instrument into a wellbore drilled through earth formations, the instrument comprising a first gravity sensor and a second gravity sensor spaced apart from the first gravity sensor;

(b) illuminating optical elements on a first mass in the first sensor, the optical elements on the first mass adapted to free fall when released, the optical elements on the first mass adapted to change a length of an optical path in response to movement of the first mass;

(c) serially illuminating optical elements on a second mass in the second sensor, the optical elements on the second mass adapted to free fall when released, the optical elements on the second mass adapted to change a length of an optical path in response to movement of the second mass, the change in length effected by movement of the second mass having a sense opposite to the change in length effected by the first mass;

(d) dropping the first mass at a first selected time;

(e) dropping the second mass at a second selected time, the dropping the second mass timed to provide at least some time coincident movement of the first mass and the second mass;

(f) splitting light traveling away from the optical elements;

(g) conducting one output of the splitting substantially directly to one input of an interferometer;

(h) conducting another output of the splitting to the interferometer through a selected time delay;

(j) determining a frequency of an interference pattern in the interferometer during the at least partially time coincident movement, the frequency related to gravity difference between a position of the first mass and a position of the second mass; and

(k) moving the instrument along the wellbore and repeating (a) through (j).

25. The method as defined in claim 24 further comprising repeating (a) through (j) at selected time intervals to determine movement of a fluid contact in a reservoir penetrated by the wellbore.

26. The method as defined in claim 25 further comprising repeating (a) through (j) at selected time intervals in a plurality of wellbores to determine spatial distribution of a fluid contact in the reservoir.

27. The method as defined in claim 24 further comprising:

prior to the splitting, directing light leaving the optical elements on the second mass to optical elements on each of a plurality of masses each adapted to free fall when selectively released from an initial position, the optical elements on each of the plurality of masses connected in optical series and adapted to change the length of the optical path in response to the dropping of each of the plurality of masses, the change in length caused by each of the plurality of masses having a sense opposite to the change in length of the previous one of the plurality of masses in the optical series;

selectively dropping each one of the plurality of masses, the selective dropping timed to provide at least partially time-coincident movement of pairs of series-adjacent ones of the plurality of masses; and

determining a frequency of an interference pattern in the interferometer in response to the time-coincident movement of the pairs series-adjacent ones of the plurality of masses, the frequency thereof corresponding to a difference in gravity between positions of each mass in each of the pairs of series-adjacent ones of the plurality of masses.

28. The method as defined in claim 24 further comprising:

determining an orientation of the logging instrument with respect to earth'"'"'s gravity; and

adjusting a measure of gravity difference between the first sensor and the second sensor with respect to a true vertical separation between the first sensor and the second sensor.

29. The method as defined in claim 24 wherein the inserting the well logging instrument is performed by extending an armored electrical cable into the wellbore.

30. The method as defined in claim 24 wherein the inserting the well logging instrument is performed by extending a drill pipe into the wellbore.

31. The method as defined in claim 24 further comprising causing light to traverse an optical path between the first mass and an optical target a plurality of times so that the change in length of the light path in the first sensor is a multiple of a distance of movement of the first mass.

32. The method as defined in claim 24 further comprising causing light to traverse an optical path between the second mass and an optical target a plurality of times so that the change in length of the light path in the second sensor is a multiple of a distance of movement of the second mass.