US 20020067164 A1 Abstract Nuclear magnetic resonance measurements on a fluid in a rock and methods of analyzing nuclear magnetic resonance data are described. At least one nuclear magnetic resonance measurement is performed, and nuclear magnetic resonance data from each of the measurements are acquired. The data are compressed and analyzed to extract information about the fluid in the rock.
Claims(21) 1. A method of extracting information about a system of nuclear spins comprising:
a) performing a plurality of nuclear magnetic resonance measurements on the system of nuclear spins; b) acquiring nuclear magnetic resonance data from each of the plurality of nuclear magnetic resonance measurements; c) expressing the nuclear magnetic resonance data using a kernel that is separable along at least two dimensions; d) compressing the nuclear magnetic resonance data along each dimension of the kernel; and e) analyzing the compressed nuclear magnetic resonance data to extract information about the system of nuclear spins. 2. The method of 3. The method of _{r}(τ_{1}, τ_{2})=∫∫k_{1}(x, τ_{1})k_{2}(y, τ_{2})f_{r }(x, y)dxdy+E_{r}(τ_{1}, τ_{2}) , where M_{r}(τ_{1}, τ_{2}) represents the nuclear magnetic resonance data; k_{1 }and k_{2 }represent the kernel separated along a first and a second dimension, respectively; τ_{1 }and τ_{2 }are a first and a second time, respectively, associated with the nuclear magnetic resonance measurement; x and y are parameters related to the system of spins; f_{r}(x, y) is a joint probability density function of x and y; and E_{r}(τ_{1}, τ_{2}) represents noise associated with the nuclear magnetic resonance data. 4. The method of _{r}=K_{1}F_{r}K_{2}′+E_{r}, where matrices K_{1 }and K_{2 }contain entries corresponding to k_{1 }and k_{2}, respectively; and F_{r }represents a discretized version Of f_{r}(x, y). 5. The method of 6. The method of 7. The method of 8. A method of extracting information about a fluid in a rock comprising:
a) applying a sequence of magnetic field pulses to the fluid, the sequence comprising a first part designed to prepare a system of nuclear spins in the fluid in a first state followed by a second part designed to generate a first series of magnetic resonance signals; b) detecting the first series of magnetic resonance signals from the fluid; c) expressing the detected magnetic resonance signals as a function having a kernel that is separable along at least two dimensions; d) compressing the detected magnetic resonance signals along each dimension of the kernel to form a compressed data set; and e) analyzing the compressed data set to extract information about the fluid in the rock. 9. The method of f) modifying the first part of the sequence; g) applying the sequence to the fluid, the modified first part being designed to prepare the system of nuclear spins in a second state and the second part generating a second series of magnetic resonance signals; and h) detecting the second series of magnetic resonance signals from the fluid. 10. The method of 11. The method of 12. The method of 13. The method of 14. The method of 15. The method of 16. The method of 17. The method of 18. The method of 19. The method of 20. A logging apparatus comprising:
a logging tool that is moveable through a borehole; and a processor coupled with the logging tool, the processor being programmed with instructions which, when executed by the processor, cause the logging tool to:
a) perform a plurality of nuclear magnetic resonance measurements on a region of investigation within an earth formation surrounding the borehole;
b) acquiring nuclear magnetic resonance data dependent on at least two dimensions from each of the plurality of nuclear magnetic resonance measurements; and
cause the processor to:
c) compress the nuclear magnetic resonance data along each of the dimensions; and
d) analyze the compressed nuclear magnetic resonance data in an optimization framework to extract information about the region of investigation.
21. The apparatus of claim 20, wherein each of the plurality of nuclear magnetic resonance measurements comprises:
applying a sequence of magnetic field pulses to a region of investigation of earth formation surrounding the borehole, the sequence comprising a first part designed to prepare a system of nuclear spins in the fluid in a first state followed by a second part designed to generate a series of magnetic resonance signals; and wherein the nuclear magnetic resonance data comprises the series of magnetic resonance signals. Description [0001] This patent application claims priority from U.S. Provisional Patent Application Ser. No. 60/220,053 filed Jul. 21, 2000, and from U.S. patent application No. 09/723,803 filed on Nov. 28, 2000, both of which are herein incorporated by reference in their entireties. [0002] This invention relates to nuclear magnetic resonance (NMR) measurements and, more particularly, analysis of NMR data. [0003] NMR has been a common laboratory technique for over forty years and has become an important tool in formation evaluation. General background of NMR well logging can be found, for example, in U.S. Pat. No. 5,023,551 to Kleinberg et al., which is assigned to the same assignee as the present invention and herein incorporated by reference in its entirety. [0004] NMR relies upon the fact that the nuclei of many chemical elements have angular momentum (“spin”) and a magnetic moment. In an externally applied static magnetic field, the spins of nuclei align themselves along the direction of the static field. This equilibrium situation can be disturbed by a pulse of an oscillating magnetic field (e.g., a RF pulse) that tips the spins away from the static field direction. The angle through which the spins are tipped is given by θ=γB [0005] After tipping, two things occur simultaneously. First, the spins precess around the direction of the static field at the Larmor frequency, given by ω [0006] Also associated with the spin of molecular nuclei is a second relaxation time, T [0007] A standard technique for measuring T [0008] In theory, other laboratory NMR measurements may be applied in well-logging to extract additional information about the oilfield, but in practice, the nature of well-logging and the borehole environment make implementing some laboratory NMR measurements difficult. For example, inversion recovery is a common laboratory technique for measuring T [0009] Accordingly, there continues to be a general need for improved NMR measurements and, in particular for the oil and gas exploration industries, improved NMR methods that can be used to extract information about rock samples and be used in well-logging applications. [0010] The invention provides a method for extracting information about a system of nuclear spins, such as in a fluid that may be contained in a rock or within a portion of earth formation surrounding a borehole (as used hereinafter, the term “rock” includes earth, earth formation, and a portion of earth formation), or other porous environment. The method involves performing at least one nuclear magnetic resonance measurement on a system of nuclear spins and acquiring nuclear magnetic resonance data from each of the measurements. The nuclear magnetic resonance data are expressed using a kernel that is separable along at least two dimensions, compressed along each dimension of the kernel, and then analyzed to extract information about the system of spins. [0011] Further details and features of the invention will become more readily apparent from the detailed description that follows. [0012] The invention will be described in more detail below in conjunction with the following Figures, in which: [0013]FIG. 1 schematically represents a magnetic field pulse sequence that may be used in accordance with the invention; [0014]FIG. 2 illustrates an inversion recovery-CPMG sequence; [0015]FIG. 3 illustrates one embodiment of a driven equilibrium-refocusing sequence according to the invention; [0016]FIGS. 4A and 4B illustrate embodiments of a diffusion editing-CPMG sequence according to the invention; [0017]FIG. 5 schematically illustrates one embodiment of a nuclear magnetic resonance measurement according to the invention; [0018]FIG. 6 schematically illustrates an alternative embodiment of a nuclear magnetic resonance measurement according to the invention; [0019]FIG. 7 contains a two-dimensional map of T [0020]FIG. 8 contains a two-dimensional map of T [0021]FIG. 9 contains a two-dimensional map of <T [0022]FIG. 10 illustrates a routine that may be used in implementing one embodiment of a method of the invention. [0023]FIG. 1 schematically represents a sequence of magnetic field pulses, such as RF pulses, that may be applied to a system of nuclear spins, such as in a fluid in a rock, in accordance with the invention. The magnetic field pulse sequence [0024] In generating the series of magnetic resonance signals, the first and second parts preferably excite spins at about the same frequency range. For example, a standard CPMG sequence with a series of 180-degree pulses tends to refocus on-resonance spins, namely those spins having a frequency substantially equal to the Larmor frequency, and the observed CPMG signal primarily includes such on-resonance spins. Accordingly, a standard CPMG sequence would be preferably paired with a first part that also primarily excites on-resonance spins. For a first part that affects primarily off resonance spins, such as a constant RF irradiation (discussed below), the second part preferably is designed to excite substantially the same off-resonance spins. A CPMG-like sequence, in which composite pulses designed to refocus the off-resonance spins replace the 180-degree pulses, may be used in such magnetic pulse sequences. Those of skill in the art will be able to design other types of refocusing sequences to refocus spins having different off-resonance frequencies. [0025] For example, FIG. 2 shows a magnetic field pulse sequence [0026] where T [0027] Another example of a magnetic field pulse sequence that may be used in accordance with the invention includes a first part that is designed to prepare the system of spins in a driven equilibrium state. In general, any magnetic field pulse sequence that repeatedly rotates the net magnetization of the system between the longitudinal and the transverse directions will create a sizable driven equilibrium magnetization. As long as the repeating magnetic field pulse units are short compared to T [0028] After the spins are prepared in a driven equilibrium, a second part designed to refocus the spins of the system is applied. The second part generates a series of magnetic resonance signals that depends on both the T [0029] T [0030] is the two dimensional density function for the ratio T [0031]FIG. 3 illustrates one example of such a driven equilibrium-refocusing sequence. The magnetic field pulse sequence [90 [0032] where t [0033] The asymptotic expression in equation (5) offers a good approximation for the DEFT driven equilibrium magnetization for all parameters in the range of about T [0034] is given by:
[0035] which is most sensitive to changes in T [0036] Another example of a driven equilibrium-refocusing magnetic field pulse sequence uses a constant RF field, typically applied for a time greater than T [0037] T [0038] which is equivalent to the DEFT equilibrium magnetization for δ [0039] Another type of magnetic field pulse sequence that may be used in accordance with the invention includes a first part that prepares a system of spins with a net magnetization that depends on a diffusion coefficient. A CPMG sequence typically follows the first part and generates a series of magnetic resonance spin echoes that generally decays according to:
[0040] where D is the diffusion coefficient, τ [0041]FIG. 5 schematically illustrates one embodiment of a nuclear magnetic resonance measurement according to the invention that involves preparing a system of spins in the fluid with different initial conditions and then measuring the decay of the spins from the different initial conditions using the same refocusing sequence. A first sequence [0042] As shown in FIG. 5, the first sequence [0043] The first sequence [0044] The same refocusing sequence [0045] The second part [0046] As shown in FIG. 5, the first sequence [0047] The magnetic resonance spin echoes generated from magnetic field pulse sequences [0048]FIGS. 7 and 8 contain a two-dimensional map of T, versus T [0049] Some embodiments of the invention may generate a large number of data points. For example, the plurality of inversion recovery-CPMG experiments described above may generate a million or more data points. To analyze NMR data that may be generated by the methods of the invention in real time and without large computer memory requirements, an inversion method has been developed that takes advantage of the tensor product structure of the kernel (see equations (1), (3) and (9) above). For example, the inversion recovery-CPMG data may be expressed with a kernel that is separable into k [0050] In implementing the inversion method, each data set is discretized and written in matrix notation: [0051] where R is the number of data sets and, for the discretized parameters x [0052] where ∥·∥ [0053] The inversion method involves first compressing the data M [0054] where {tilde over (K)} is the tensor product of {tilde over (K)} [0055] As mentioned previously, the smoothening parameter α controls the smoothness of the estimated density function F [0056] This inversion method may be applied to any two- to three-dimensional NMR data that may be expressed generally as: [0057] where M [0058] The inversion recovery-CPMG measurements in conjunction with the inversion method described above is capable of providing a full map of the two-dimensional density function, f(T [0059] For example, a driven equilibrium-refocusing sequence as described above prepares the system of spins with an equilibrium magnetization that depends on T [0060]FIG. 9 illustrates a two-dimensional map of <T [0061] was obtained, from which <T [0062] The DEFT-CPMG sequence used to generate the <T [0063] In inhomogeneous fields such as is typically found in most well-logging applications, however, some spins are necessarily off-resonance, and, in the fast pulsing limit (i.e., τ [0064] It should be noted that the constant RF irradiation driven equilibrium, being generated by a single pulse, would not be as sensitive to pulse mismatches and pulse imperfections as the DEFT driven equilibrium, and so is well-suited for use with inhomogeneous fields, such as are found in most well-logging applications. [0065] The invention may be implemented in well logging using any nuclear magnetic resonance (NMR) well logging apparatus known in the art. Embodiments of the invention may be implemented with NMR well logging devices without the need for hardware modifications. FIG. 10 shows a flow diagram of a routine that can be used in programming a processor in implementing certain embodiments of the invention. The routine may be stored on or provided over a computer or machine readable medium, such as read-only memory (ROM); random access memory (RAM); magnetic disc or tape; a CD-ROM or other optical storage media; electrical, optical, acoustical or other forms of propagated signals; and the like. The processor may be a downhole processor, an uphole processor, or a combination thereof. The processor also may include a remote processor that may be used for implementing some of the data inversion and interpretation parts of the routine. [0066] Prior to the beginning of the programmed routine and as shown at [0067] The programmed routine begins at block [0068] Some embodiments of the invention involve repeatedly applying the magnetic field pulse sequence, or involve applying a plurality of magnetic field pulse sequences. A parameter R may be used (set, perhaps, at block [0069] The data inversion begins at block [0070] The invention allows information about a system of nuclear spins, such as in a fluid in a rock, to be extracted, either in a laboratory setting or in well-logging applications. Some embodiments may be used to extract two-dimensional maps of parameters of interest, such as T Referenced by
Classifications
Legal Events
Rotate |