Two-dimensional magnetic resonance imaging in a borehole

• US 6,522,137 B1
• Filed: 06/28/2000
• Issued: 02/18/2003
• Est. Priority Date: 06/28/2000
• Status: Expired due to Term

• Current Assignee: Schlumberger Technology Corporation (SLB)
• Original Assignee: Schlumberger Technology Corporation (SLB)
• Inventors: Sun, Boqin, Taherian, Reza, Crary, Steven F., Sezginer, Abdurrahman
• Primary Examiner(s): Lefkowitz, Edward
• Assistant Examiner(s): Fetzner, Tiffany A.
• Application Number:
  US09/605,805
• Time in Patent Office: 965 Days
• Field of Search: 324/303, 324/309, 324/300, 324/306, 175/45
• US Class Current: 324/303
• CPC Class Codes: G01N 24/081 Making measurements of geologic samples, e.g. measurements of moisture, pH, porosity, permeability, tortuosity or viscosity
• CPC Class Codes: G01V 3/32 operating with electron or nuclear magnetic resonance

Abstract

A downhole NMR measurement apparatus for use in a borehole includes at least one magnet, at least one RF transmission coil, at least one gradient coil and circuitry. The magnet(s) establish a magnetic field in a region of a formation that at least partially surrounds the measurement apparatus. The RF transmission coils(s) transmit RF pulses pursuant to an NMR pulse sequence into the region to, in combination with the magnetic field, induce the generation of spin echo signals from a resonance volume within the region. The gradient coil(s) establish a pulsed gradient field in the resonance volume, and the circuitry is coupled to the gradient coil(s) to control the generation of the pulsed gradient field to phase encode the spin echo signals for purposes of high resolution imaging of the formation.

Claims

1. A method usable with a downhole NMR measurement apparatus, comprising

using a magnet to polarize spins in a downhole formation that surrounds the NMR measurement apparatus;

transmitting RF pulses pursuant to an NMR pulse sequence into the downhole formation;

in response to the RP pulses, receiving spin echo signals from a region of the formation;

generating a pulse gradient field in the downhole formation;

controlling the generation of the pulsed gradient field to phase encode the spin echo signals; and

imaging at least one formation evaluation characteristic, independent of fluid flow within the formation, based on the phase encoded spin echo signals for at least a two-dimensional region of the downhole formation that circumscribes the NMR measurement apparatus.

2. The method of claim 1, wherein the generating the pulsed gradient field comprises:

progressively increasing a magnitude of the pulsed gradient field.

3. The method of claim 1, wherein the generating the pulsed gradient field comprises:

pulsing at least one gradient coil with a current.

4. The method of claim 1, wherein

the NMR pulse sequence comprises successive refocusing pulses, each refocusing pulse producing a spin echo signal that precedes the next successive refocusing pulse in time;

and

generating the pulsed gradient field comprises;

for every other spin echo signal, pulsing at least one gradient coil with a current before said every other spin echo signal and after the last refocusing pulse and pulsing said at least one gradient coil with the current after said every other spin echo signal and before the next refocusing pulse.

5. The method of claim 1, wherein the pulsed gradient field is approximately tangential to the NMR measurement apparatus.

6. The method of claim 1, wherein the pulsed gradient is approximately along an axis of the borehole.

7. The method of claim 1, wherein generating the pulsed gradient field comprises:

pulsing at least one first gradient coil with a first current to produce a first gradient field; and

pulsing at least one second gradient coil with a second current to produce a second gradient field that varies in a substantially different direction to the first gradient field.

8. The method of claim 1, further comprising:

using the phase encoded spin echo signals to form an image of the borehole.

42. The method of claim 8 wherein the NMR measurement apparatus forms part of a drilling tool string and all of said method is performed while moving the drilling string along a wellbore traversing the downhole formation.

9. A downhole NMR measurement device for use in a borehole, comprising:

at least one magnet to establish a magnetic field in a region of a formation that at least partially surrounds the measurement device;

at least one RF transmission coil to transmit RF, pulses pursuant to an NMR pulse sequence into the region to, in combination with the magnetic field, induce the generation of spin echo signals from a resonance volume within the region;

at least one gradient coil to generate a pulsed gradient field in the resonance volume; and

circuitry coupled to said at least one gradient coil to control the generation of the pulsed gradient field to phase encode the spin echo signals, wherein the phase encoded spin echo signals are spatially located and are used to image in at least two dimensions at least one formation evaluation characteristic, independent of fluid flow within the formation, for a region of the formation that at least partially circumscribes the measurement device.

10. The NMR measurement apparatus of claim 9, wherein

said at least one gradient coil comprises multiple gradient coils to establish a first gradient field component along a first direction and a second gradient field component along a second direction to combine with the first gradient field component to establish the gradient field in a direction of interest.

11. The NMR measurement apparatus of claim 10, wherein the multiple gradient coils comprises coil portions that are equally spaced about a longitudinal axis of the measurement apparatus and extend along the longitudinal axis near an outer surface of the magnet.

12. The NMR measurement apparatus of claim 10, wherein

said at least one magnet has a first surface near a first end and a second surface near a second opposite end, a longitudinal axis of the measurement apparatus extending through the first and second surfaces;

the multiple gradient coils comprise first coil portions located near the first surface of said at least one magnet and second coil portions located near the second surface of said at least one magnet.

13. The NMR measurement apparatus of claim 12, wherein at least some of the first and second coil portions are arc-shaped.

14. The NMR measurement apparatus of claim 10, wherein said at least one magnet comprises a circularly cylindrical magnet polarized across its diameter.

15. The NMR measurement apparatus of claim 10, wherein said at least one magnet comprises a circularly cylindrical magnet polarized across its longitudinal axis.

16. The NMR measurement apparatus of claim 10, wherein

said at least one magnet comprises a first magnet polarized in a first direction along a longitudinal axis of the NMR measurement apparatus and a second magnet polarized in a second opposite direction along the longitudinal axis;

and

the multiple gradient coils comprise a first gradient coil located between the first and second magnets to establish the first gradient component and a second gradient coil located between the first and second magnets to establish the second gradient component.

17. The NMR measurement apparatus of claim 9, wherein the gradient field varies with a longitudinal axis of the tool, said at least one gradient coil comprises:

a first set of gradient coils located near first surfaces of said at least one magnet to add to the magnetic field to create a positive gradient component of the gradient field; and

a second set of gradient coils located near second surfaces of said at least one magnet to subtract from the magnetic field to create a negative gradient component of the gradient field.

18. The NMR measurement apparatus of claim 9, wherein the gradient field varies with a longitudinal axis of the tool, said at least one gradient coil comprises:

a first gradient coil located near a first end of said at least one magnet to add to the magnetic field to create a positive gradient component of the gradient field; and

a second gradient coil located near a second end of said at least one magnet opposite from the first end to subtract from the magnetic field to create a negative gradient component of the gradient field.

19. The NMR measurement apparatus of claim 9, wherein the spin echo signals are localized to different parts of the region, the apparatus further comprising:

surface pads spaced around a longitudinal axis of the measurement apparatus and positioned near a wall of the borehole; and

arrays of RF coils, each array attached to a different surface pad for measuring the spin echo signals localized to one of the parts of the region near the attached surface pad.

20. The NMR measurement apparatus of claim 19, wherein the RF coils of at least one of the arrays are arranged in rows and columns.

21. The NMR measurement apparatus of claim 19, wherein the circuitry is further adapted to use the arrays for purposes of tangential imaging of the formation about a longitudinal axis of the measurement apparatus.

22. The NMR measurement apparatus of claim 21, wherein the circuitry is further adapted to use a gradient field for the purpose of tangential imaging.

23. The NMR measurement apparatus of claim 21, wherein the circuitry is further adapted to not use a gradient field for the purpose of longitudinal imaging.

24. The NMR measurement apparatus of claim 19, wherein the circuitry is further adapted to use the array of coils as receivers and use at least one larger RF transmission coil.

25. The NMR measurement apparatus of claim 9, wherein the circuitry is further adapted to increase a magnitude of the gradient field.

26. The NMR measurement apparatus of claim 9, wherein the circuitry is further adapted to pulse said at least one gradient coil with a current between the reception of spin echo signals.

27. The NMR measurement apparatus of claim 9, wherein

the NMR pulse sequence comprises successive refocusing pulses, each refocusing pulse producing a spin echo signal that precedes the next successive refocusing pulse in time;

and

the circuitry is further adapted to;

for every other spin echo signal, pulse at least one gradient coil with a current before said every other spin echo signal and after the last refocusing pulse and pulse said at least one gradient coil with the current after said every other spin echo signal and before the next refocusing pulse.

28. The NMR measurement apparatus of claim 9, wherein the circuitry is further adapted to vary the pulsed gradient field approximately tangentially around the borehole.

29. The NMR measurement apparatus of claim 9, wherein the circuitry is further adapted to vary the pulsed gradient field approximately along an axis of the borehole.

30. The NMR measurement apparatus of claim 9, wherein the circuitry is further adapted to:

pulse at least one first gradient coil with a first current; and

pulse at least one second gradient coil with a second current.

31. An NMR measurement device apparatus for use downhole comprising:

at least one magnet to establish a magnetic field in a region of a formation that at least partially surrounds the measurement device;

at least one RF transmission coil to transmit RF pulses pursuant to an NMR pulse sequence into the region to, in combination with the magnetic field, induce the generation of spin echo signals from a resonance volume within the region, the spin echo signals being localized to different parts of the region,

surface pads spaced around a longitudinal axis of the measurement apparatus and positioned near a wall of the borehole; and

arrays of RF receiving coils, each array attached to a different surface pad for measuring the spin echo signals localized to one of the parts of the region near the attached surface pad, wherein the spin echo signals are spatially located and are used to image in at least two-dimensions at least one formation evaluation characteristic, independent of fluid flow within the formation, for the region of the formation that at least partially circumscribes the measurement device.

32. The NMR measurement apparatus of claim 31, wherein the RF receiving coils of at least one of the arrays are arranged in rows and columns.

33. The NMR measurement apparatus of claim 31, wherein the circuitry is further adapted to use the arrays for purposes of tangential imaging of the formation about a longitudinal axis of the measurement apparatus.

34. The NMR measurement apparatus of claim 31, further comprising:

circuitry adapted to use the RF coils as receiver antennas only; and

at least one RF transmission coil.

35. A method usable with a downhole NMR measurement device apparatus, comprising:

producing spin echo signals in a downhole formation;

phase encoding the spin echo signals; and

using the phase encoded spin echo signals to obtain at least a two-dimensional image of at least one formation evaluation characteristic, independent of fluid flow within the formation, of the downhole formation that circumscribes the measurement device.

36. The method of claim 35, wherein the image comprises a high resolution image.

37. The method of claim 35, wherein the producing comprises:

using a magnet to polarize spins in a downhole formation that surrounds the NMR measurement apparatus; and

transmitting RF pulses pursuant to an NMR pulse sequence into the downhole formation.

38. The method of claim 35, wherein the phase encoding the spin echo signals comprises:

progressively increasing a magnitude of a pulsed gradient field.

39. The method of claim 35, wherein the phase encoding the spin echo signals comprises:

pulsing at least one gradient coil with a current.

40. The method of claim 35, wherein

producing the spin echo signals comprises transmitting an NMR pulse sequence,

the NMR pulse sequence comprises successive refocusing pulses, each refocusing pulse producing a spin echo signal that precedes the next successive refocusing pulse in time;

and

the phase encoding the spin echo signals comprises;

for every other spin echo signal, pulsing at least one gradient coil with a current before said every other spin echo signal and after the last refocusing pulse and pulsing said at least one gradient coil with the current after said every other spin echo signal and before the next refocusing pulse.

41. The method of claim 35, wherein the producing the phase encoded spin echo signals comprises:

pulsing at least one first gradient coil with a first current to produce a first gradient field; and

pulsing at least one second gradient coil with a second current to produce a second gradient field that varies in a substantially different direction to the first gradient field.

43. The method of claim 35 wherein the NMR measurement apparatus forms part of a drilling tool string and all of said method is performed while moving the drilling string along a wellbore traversing the downhole formation.