Methods and systems for determining angular orientation of a drill string

• US 20060260843A1
• Filed: 05/01/2006
• Published: 11/23/2006
• Est. Priority Date: 04/29/2005
• Status: Active Grant

• Current Assignee: Martin E. Cobern
• Original Assignee: APS Technology Inc
• Inventors: Cobern, Martin E.
• Granted Patent: US 7,681,663 B2
• Time in Patent Office: Days
• US Class Current: 175/45
• CPC Class Codes: E21B 47/024 of devices in the borehole determining slope or direction of the borehole E21B47/022

Abstract

Preferred methods and systems generate a control input based on a periodically-varying characteristic associated with the rotation of a drill string. The periodically varying characteristic can be correlated with the magnetic tool face and gravity tool face of a rotating component of the drill string, so that the control input can be used to initiate a response in the rotating component as a function of gravity tool face.

Claims

1. A method, comprising:

causing a drill string to rotate within an earth formation;

monitoring a magnetic field as the drill string rotates;

generating an electrical signal in response to a periodically-varying characteristic of the magnetic field; and

sending the electrical signal to a component of the drill string that is responsive to the electrical signal.

2. The method of claim 1, further comprising:

determining gravity tool face and magnetic tool face of the component of the drill while the component of the drill string is not rotating;

calculating a difference between the gravity tool face and magnetic tool face determined while the component of the drill string is not rotating;

calculating a first angular position corresponding to a difference between an angular position at which a response of the component of the drill string is to occur, and the difference between the gravity tool face and magnetic tool face determined while the component of the drill string is not rotating; and

timing the generation of the electrical signal based on the difference between the angular position at which a response of the component of the drill string is to occur, and the difference between the gravity tool face and magnetic tool face determined while the component of the drill string is not rotating.

3. The method of claim 2, further comprising:

calculating an angular velocity of the component of the drill string based on a period of rotation of the component;

calculating a time required for the component of the drill string to rotate from a second angular position at which the periodically-varying characteristic of the magnetic field occurs, to the first angular position based on the angular velocity; and

generating the electrical signal based on the time required for the component of the drill string to rotate from the second angular position to the first angular position.

4. The method of claim 3, wherein the magnetic tool face of the component of the drill string is approximately zero when the component of the drill string is in the second position.

5. The method of claim 3, wherein the periodically-varying characteristic of the magnetic field is a measurement of a component of a local geomagnetic field as measured by a magnetometer that rotates with the drill string.

6. The method of claim 5, wherein the periodically-varying characteristic of the magnetic field is a zero value for the component of the local geomagnetic field.

7. The method of claim 3, wherein generating the electrical signal based on the time required for the component of the drill string to rotate from the second angular position to the first angular position comprises generating the electrical signal approximately when the time required for the component of the drill string to rotate from the second angular position to the first angular position elapses after the component of the drill string is in the second angular position.

8. The method of claim 3, wherein generating the electrical signal based on the time required for the component of the drill string to rotate from the second angular position to the first angular position comprises:

calculating a quantity of time equal to a difference between a response time of the component of the drill string to the electrical signal and the time required for the component of the drill string to rotate from the second angular position to the first angular position; and

generating the electrical signal approximately when the quantity of time elapses after the component of the drill string is in the second angular position.

9. The method of claim 1, wherein sending the electrical signal to a component of the drill string that is responsive to the electrical signal comprises sending the electrical signal to the component of the drill string to cause an arm of the component of the drill string to extend and push against the earth formation thereby steering the drill string.

10. The method of claim 9, wherein the component of the drill string is a rotary steerable motor.

11. The method of claim 5, wherein the magnetometer is mounted on the component of the drill string at approximately the same angular position as a portion of the component of the drill string that is responsive to the electrical signal.

12. The method of claim 5, wherein the magnetometer is mounted on the drill string up-hole of the component of the drill string.

13. The method of claim 12, further comprising calculating a difference between an angular position of the magnetometer and an angular position of a portion of the component of the drill string that is responsive to the electrical signal;

wherein the first angular position further corresponds to the difference between the angular position at which the response of the component of the drill string is to occur, and the difference between the angular position of the magnetometer and the angular position of the portion of the component that is responsive to the electrical signal.

14. The method of claim 6, wherein calculating the angular velocity of the component of the drill string based on the period of rotation of the component of the drill string comprises calculating the angular velocity of the component of the drill string based on a periodic occurrence of the zero value for the component of the local geomagnetic field.

15. The method of claim 6, wherein calculating the angular velocity of the component of the drill string based on the period of rotation of the component of the drill string comprises calculating the angular velocity of the component of the drill string based on four periodic occurrences of the zero value for the component of the local geomagnetic field.

16. The method of claim 2, further comprising calculating the angular position at which the response of the component of the drill string is to occur by calculating a difference between a desired heading along which the drill string is to be steered and 180°

.

17. A method, comprising:

drilling a subsurface bore using a rotating drill string;

calculating a time required for a rotating component of the drill string to rotate through an angular displacement approximately equal to an angular distance between a first angular position of the rotating component, and a second angular position of the rotating component at which a predetermined response of the rotating component is occur;

determining when the rotating component reaches the first angular position by measuring a quantity that varies with the angular position of the rotating component; and

monitoring the time that elapses after the rotating component reaches the first angular position.

18. The method of claim 17, wherein the quantity that varies with the rotation of the rotating component varies periodically with the rotation of the drill string.

19. The method of claim 17, wherein the quantity that varies with the rotation of the rotating component is a component of a magnetic field measured by a magnetometer that rotates with the rotating component.

20. The method of claim 17, further comprising sending a control input to the rotating component to cause the predetermined response of the rotating component to take place when the rotating component is located approximately at the second position.

21. The method of claim 20, further comprising sending the control input to the rotating component approximately when the time required for the rotating component to translate through the angular distance elapses after the rotating component reaches the first angular position.

22. The method of claim 20, further comprising:

calculating a time interval equal to a difference between the time required for the rotating component to translate through the angular distance and a response time of the rotating component to the control input; and

sending the control input to the rotating component approximately when the time interval elapses after the rotating component reaches the first angular position.

23. The method of claim 18, further comprising:

determining gravity tool face and magnetic tool face of the component while the rotating component is not rotating;

calculating a difference between the gravity tool face and magnetic tool face determined while the rotating component is not rotating; and

determining the second angular position by calculating a difference between an angular position at which a response of the rotating component is to occur, and the difference between the gravity tool face and magnetic tool face determined while the rotating component is not rotating.

24. The method of claim 17, further comprising:

calculating an angular velocity of the rotating component based on a period of rotation of the rotating component; and

calculating the time required for a rotating component of the drill string to rotate through the angular displacement based on the angular velocity of the rotating component.

25. The method of claim 23, wherein the magnetic tool face of the component is approximately zero when the component is in the first position.

26. The method of claim 19, wherein the component of the magnetic field measured by the magnetometer is approximately zero when the rotating component is in the first position.

27. The method of claim 20, wherein sending a control input to the rotating component to cause the predetermined response of the rotating component to take place when the rotating component is located approximately at the second position comprises sending the control input electrical to cause an arm of the rotating component to extend and push against the earth formation thereby steering the drill string.

28. The method of claim 27, wherein the rotating component is a rotary steerable motor.

29. The method of claim 19, wherein the magnetometer is mounted on the rotating component at approximately the same angular position as a portion of the rotating component that is responsive to the control input.

30. The method of claim 19, wherein the magnetometer is mounted on the rotating component up hole of the rotating component.

31. The method of claim 24, wherein calculating an angular velocity of the rotating component based on a period of rotation of the rotating component comprises calculating the angular velocity of the rotating component based on a periodic occurrence of a zero value for a value of a magnetic field measured by a magnetometer that rotates with the rotating component.

32. The method of claim 24, wherein calculating an angular velocity of the rotating component based on a period of rotation of the rotating component comprises calculating the angular velocity of the rotating component based on four periodic occurrences of a zero value for a value of a magnetic field measured by a magnetometer that rotates with the rotating component.

33. The method of claim 23, further comprising calculating the angular position at which the response of the component is to occur by calculating a difference between a desired heading along which the drill string is to be steered and 180°

.

34. A method, comprising:

determining gravity tool face and apparent magnetic tool face of a rotatable component while the rotatable component is not rotating;

determining an offset between the gravity tool face and the apparent magnetic tool face;

determining a first angular position by calculating a difference between the offset and an angular position at which a desired action of the rotatable component is to take place;

measuring a component of a geomagnetic field around the rotatable component while the rotatable component is rotating;

calculating an angular distance between the first angular position and a second angular position at which a measured value of the geomagnetic field is approximately zero; and

calculating a time required for the rotatable component to rotate from the second angular position to the first angular position.

35. The method of claim 34, further comprising sending an electrical signal to the rotatable component to cause a response to occur approximately when the time required for the rotatable component to rotate from the first angular position to the second angular position elapses after the rotatable component is in the first angular position.

36. The method of claim 34, wherein magnetic tool face is approximately zero when the rotatable component is in the second angular position.

37. A system, comprising:

at least two accelerometers that measure components of a gravitational field around a rotatable component of a drill string;

a two or three-axis magnetometer that measures components of a magnetic field around the rotatable component; and

a controller communicatively coupled to the accelerometer and the magnetometer, wherein the controller generates an electrical signal in response to a periodically-varying characteristic of the magnetic field, and sends the electrical signal to a component of the drill string that is responsive to the electrical signal.

38. The system of claim 37, wherein the controller determines gravity tool face and magnetic tool face of the component while the component is not rotating;

calculates a difference between the gravity tool face and magnetic tool face determined while the component is not rotating; and

calculates a first angular position corresponding to a difference between an angular position at which a response of the component is to occur, and the difference between the gravity tool face and magnetic tool face determined while the component is not rotating.

39. The system of claim 38, wherein the controller calculates an angular velocity of the component based on a period of rotation of the component;

calculates a time required for the component to rotate from a second angular position at which the periodically-varying characteristic of the magnetic field measurement occurs, to the first angular position based on the angular velocity; and

generates the electrical signal based on the time required for the component to rotate from the second angular position to the first angular position.

40. The method of claim 39, wherein the magnetic tool face of the component is approximately zero when the component is in the second position.

41. The method of claim 37, wherein the periodically-varying characteristic of the magnetic field is a zero value for the component of the magnetic field.

42. The system of claim 37, further comprising the component.

43. The system of claim 42, wherein the component is a rotary steerable motor.

44. The system of claim 42, wherein an arm of the component extends and pushes against an earth formation thereby steering the drill string in response to the electrical signal.

45. The system of claim 42, wherein the controller is mounted on the component, and the magnetometer is mounted on the component at approximately the same angular position as a portion of the component that is responsive to the electrical signal.

46. The system of claim 42, wherein the magnetometer and the controller are mounted up hole of the component.

47. The system of claim 37, further comprising a second controller mounted up hole of the telemetry system and communicatively coupled to the accelerometer, and a telemetry system that communicatively couples the first and second controllers.