Abstract:
A method for determining the nuclear magnetic resonance longitudinal magnetization decay of formations surrounding an earth borehole that involves: providing a logging device moveable through the borehole; applying a static magnetic field in the formations to align spins in the formations in the direction of the static magnetic field; producing a tipping pulse for tipping the direction of the spins with respect to the static magnetic field direction; and detecting the time varying magnitude of the spin magnetization as the magnetization returns toward the static magnetic field direction; the longitudinal magnetization decay being determinable from the detected time varying magnitude of the spin magnetization. Related methods and apparatus for implementing these methods are also described.

Description:
FIELD OF THE INVENTION 
     This invention relates to determination of nuclear magnetic resonance properties of formations surrounding an earth borehole and, more particulary, to a well logging method and apparatus for determining the nuclear magnetic resonance longitudinal magnetization decay of formations surrounding an earth borehole. 
     The longitudinal relaxation time constant of the formations, and/or the distribution thereof, can be obtained from the longitudinal magnetization decay. 
     BACKGROUND OF THE INVENTION 
     General background of nuclear magnetic resonance (NMR) well logging is set forth, for example, in U.S. Pat. No. 5,023,551. Briefly, in conventional NMR operation the spins of nuclei align themselves along an externally applied static magnetic field. This equilibrium situation can be disturbed by a pulse of an oscillating magnetic field (e.g. an RF pulse), which tips the spins away from the static field direction. After tipping, two things occur simultaneously. First, the spins precess around the static field at the Larmor frequency, given by ω 0 =γB 0 , where B 0  is the strength of the static field and γ is the gyromagnetic ratio. Second, the spins return to the equilibrium direction according to a decay time T 1 , which is called the longitudinal relaxation time constant or spin lattice relaxation time constant. For hydrogen nuclei, γ/2π=4258 Hz/Gauss, so, for example, for a static field of 235 Gauss, the frequency of precession would be 1 MHz. Also associated with the spin of molecular nuclei is a second relaxation time constant, T 2 , called the transverse relaxation time constant or spin-spin relaxation time constant. At the end of a ninety degree tipping pulse, all the spins are pointed in a common direction perpendicular to the static field, and they all precess at the Larmor frequency. The net precessing magnetization decays with a time constant T 2  because the individual spins rotate at different rates and lose their common phase. At the molecular level, dephasing is caused by random motions of the spins. The magnetic fields of neighboring spins and nearby paramagnetic centers appear as randomly fluctuating magnetic fields to the spins in random motion. In an inhomogeneous field, spins at different locations precess at different rates. Therefore, in addition to the molecular spin-spin relaxation of fluids, spatial inhomogeneities of the applied field also cause dephasing. Spatial inhomogeneities in the field can be due to microscopic inhomogeneities in the magnetic susceptibility of rock grains or due to the macroscopic features of the magnet. 
     A widely used technique for acquiring NMR data, both in the laboratory and in well logging, uses an RF pulse sequence known as the CPMG (Carr-Purcell-Meiboom-Gill) sequence. As is well known, after a wait time that precedes each pulse sequence, a ninety degree pulse causes the spins to start precessing. Then a one hundred eighty degree pulse is applied to cause the spins which are dephasing in the transverse plane to refocus. By repeatedly refocusing the spins using one hundred eighty degree pulses, a series of “spin echoes” appear, and the train of echoes is measured and processed. The transverse relaxation time constant, T 2 , or the distribution of T 2 &#39;s, can be obtained using this technique. The determination of the longitudinal magnetization decay and of T 1 , however, remains difficult. A source of this difficulty is the very low signal-to-noise ratio inherent in detecting the feeble magnetic moment of nuclei. 
     The traditional pulse method of measuring the longitudinal relaxation time constant (T 1 ) is the so-called inversion recovery method (see Carr et al., Phys. Rev. 94, 630 (1954)). In this method, a 180 degree pulse is applied to a nuclear spin system, followed by a recovery time and then a 90 degree read-out pulse. The amplitude at a convenient point on the resulting free induction decay is measured, and the spin system is then allowed to recover to equilibrium by waiting approximately five times T 1  before applying the next two-pulse sequence. Many such cycles are required since the spin-lattice relaxation time is found by correlating the various recovery times with the associated free induction decay (FID) amplitudes. While this technique can provide an accurate measure of T 1  (and, with further processing, the T 1  distribution), the pulse sequence is very time consuming. 
     It is among the objects of the present invention to provide an apparatus and method that can determine the longitudinal magnetization decay and relaxation time constant of formations surrounding an earth borehole, with improved time and cost efficiency. 
     SUMMARY OF THE INVENTION 
     A form of the present invention provides a well logging technique and apparatus whereby the longitudinal magnetization decay and the longitudinal relaxation time constant (T 1 ) of formations surrounding an earth borehole can be measured directly after a single RF pulse or other suitable perturbation in direction and/or magnitude of the magnetization of the spins. In embodiments of this form of the invention, the longitudinal magnetism (that is, magnetism parallel to the static magnetic field) is sensed, in general, by a magnetic flux detector, and specifically by a superconducting flux detector. SQUIDs are the most sensitive flux detectors, but there are other flux detectors (flux gate magnetometers, conventional coils and amplifiers, etc.) which can, in principle, be used. 
     Superconductors have been employed in the design of electromagnetic sensors that are extremely sensitive. The heart of a superconducting sensor is the Superconducting Quantum Interferometric Device (SQUID), which can be envisioned as a very sensitive converter of magnetic flux to voltage. Typically, a measurement circuit will be arranged so that the detected signal results in a current flow in a loop that is inductively coupled to the SQUID. SQUIDs do not generate high fields, and they do not carry high currents. They are mechanically robust and compact, and are therefore relatively easy to cool. SQUIDs have been proposed for use in borehole logging but have not become commercially prevalent for a number of reasons, one such reason being the difficulty of devising suitable and practical logging applications for SQUIDs. [See, for example, J. Jackson, New NMR Well Logging/Fracture Mapping Technique With Possible Application Of SQUID NMR Detection, Soc. Of Explor. Geo., Tulsa, Okla., pp. 161-165, 1981.] 
     In accordance with an embodiment of the method of the invention, there is disclosed a technique for determining the nuclear magnetic resonance longitudinal magnetization decay of formations surrounding an earth borehole, comprising the following steps: providing a logging device that is moveable through the borehole; applying, from the logging device, a static magnetic field in the formations to align spins in the formations in the direction of the static magnetic field; producing, from the logging device, a tipping pulse for tipping the direction of the spins with respect to the static magnetic field direction; and detecting, at the logging device, the time varying magnitude of the spin magnetization as said magnetization returns toward the static magnetic field direction; the longitudinal magnetization decay being determinable from the detected time varying magnitude of the spin magnetization. [As background, see Sager, Kleinberg, and Wheatley, Phys. Rev. Lett., 39, 1345 (1977), and Sager, Kleinberg, and Wheatley, J. Low Temp. Phys. 32, 263 (1978), regarding laboratory application of SQUID detected signals using a 180 degree pulse and monitoring of longitudinal magnetization for NMR investigation of  3 He.] 
     In a preferred embodiment of the method of the invention, the step of detecting the time varying magnitude of the spin magnetization includes providing a magnetic flux detection system for producing a number of output signals representative of successively sampled values of the magnetic flux over a period of time. The magnetic flux detection system includes a magnetic flux detection sensor (or antenna), and a magnetic flux sensing circuit that preferably includes a SQUID. In a form of the preferred embodiment, at least part of the magnetic flux detection system is in a cooled enclosure. 
     In accordance with a feature of an embodiment of the invention, an all-metal pressure-tight housing is provided for the flux detection system. This facilitates thermal shielding (e.g. vacuum dewaring) for cooled components, and is possible because the quasistatic nature of the signal (a few hundred Hertz bandwidth) is below the frequency at which the metal housing becomes opaque to magnetic fields. For higher frequency operation, the portion of the metal housing in front of the flux detection antenna (e.g. receiver coil) can have a reduced wall thickness. 
     Further features and advantages of the invention will become more readily apparent from the following detailed description when taken in conjunction with the accompanying drawings. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a schematic diagram, partially in block form, of an apparatus that can be used in practicing embodiments of the invention. 
     FIG. 2 is a diagram of the front borehole wall-engaging face of an embodiment of the logging device of FIG. 1, which can be used in practicing embodiments of the invention. 
     FIG. 3 is a perspective view of an embodiment of one of the RF antennas of the FIG. 2 embodiment. 
     FIG. 4 is a block diagram of downhole circuitry in accordance with an embodiment of the invention. 
     FIG. 5 is a block diagram of a portion of downhole circuitry in accordance with another embodiment of the invention. 
     FIG. 6, which includes FIGS. 6A,  6 B and  6 C, show plots of magnetization versus time that are useful in understanding operation of an embodiment of the invention. 
     FIG. 7, which includes FIGS. 7A,  7 B and  7 C, show other plots of magnetization versus time that are useful in understanding operation of another embodiment of the invention. 
     FIG. 8, which includes FIGS. 8A and 8B, show further plots of magnetization versus time that are useful in understanding operation of a further embodiment of the invention. 
     FIG. 9 is a cross-sectional view of an apparatus that can be used in practicing a further form of the invention. 
    
    
     DETAILED DESCRIPTION 
     Referring to FIG. 1, there is shown an apparatus for investigating subsurface formations  31  traversed by a borehole  32 , which can be used in practicing embodiments of the invention. A magnetic resonance investigating apparatus or logging device  30  is suspended in the borehole  32  on an armored cable  33 , the length of which substantially determines the relative depth of the device  30 . The length of cable  33  is controlled by suitable means at the surface such as a drum and winch mechanism (not shown). Surface equipment, represented at  7 , can be of conventional type, and can include a processor subsystem and communicates with the all the downhole equipment. It will be understood that processing can be performed downhole and/or uphole, and that some of the processing may be performed at a remote location. Also, while a wireline is illustrated, alternative forms of physical support and communicating link can be used, for example in a measurement while drilling system. As described for example in the U.S. Pat. No. 5,055,787, the magnetic resonance logging device  30  has a face  14  shaped to intimately contact the borehole wall, with minimal gaps or standoff. The borehole wall may have a mudcake  16  thereon. A retractable arm  15  is provided which can be activated to press the body of the tool  13  against the borehole wall during a logging run, with the face  14  pressed against the wall&#39;s surface. Although the tool  13  is shown as a single body, the tool may alternatively comprise separate components such as a cartridge, sonde or skid, and the tool may be combinable with other logging tools. 
     The diagram of FIG. 2 shows the front face of the logging device  30  that abuts the borehole wall. In the embodiment of FIG. 2, a pair of spaced-apart permanent magnets  17 A and  17 B are provided. The magnets can be, for example, samarium-cobalt magnets, and can have the general configuration and polarity as shown in the above-referenced U.S. Pat. No. 5,055,787. A pair of RF antennas  18 A and  18 B are provided between the permanent magnets  17 A and  17 B. Each of the RF antennas can have the general type of configuration shown in the above-referenced &#39;787 patent; that is, an elongated trough antenna. However, whereas the &#39;787 patent illustrates one such RF antenna and uses the single RF antenna for both transmitting and receiving, the present embodiment hereof utilizes the two longitudinally aligned and spaced apart RF antennas  18 A and.  18 B for transmitting RF electromagnetic energy, and utilizes a pick-up loop antenna  21 , located between the antennas  18 A and  18 B, for receiving NMR signals from the formations. [The present invention can also operate with a single transmitting antenna. However, the plurality of transmitting antennas can provide certain operational advantages, to be treated subsequently.] As will be described further hereinbelow, the loop antenna  21  is preferably part of a magnetic flux detection system, at least part of which comprises superconducting components. Magnets  17 A and  17 B produce a static magnetic field B 0  in regions surrounding the tool  13 . The antenna(s)  18  produces, at selected times to be described, an oscillating magnetic field B 1  which is focussed into formation  12 , and is superposed on the static field B 0  within those parts of the formation opposite the face  14 . The “volume of investigation” of the tool for this embodiment, represented generally by the dashed line region  9  in FIG. 1, is a vertically elongated region directly in front of tool face  14 . 
     As described in the referenced U.S. Pat. No. 5,055,787, the two permanent magnets  17 A and  17 B can be mounted generally parallel to each other within a metal alloy body, the body being formed of a material having low magnetic permeability, so as to not interfere with the static magnetic field. The magnets  17 A and  17 B can be slab magnets which are elongated in the longitudinal direction of the borehole. The magnetic poles of each magnet are not on the smallest faces of the slab, commonly viewed as the ends of a bar magnet. Instead, the poles appear on the two opposing edges of the slab magnet. Therefore, within the formation, the magnetic field B 0  surrounding the magnets remains fairly constant along the longitudinal direction of the borehole axis. One or more further permanent magnets can also be used in this embodiment. 
     As described in the referenced &#39;787 patent, the metal body holding the permanent magnets can have, on the front face thereof, a semi-cylindrically shaped cavity or slot which faces the formations and is adapted for receiving an RF antenna (two of them, in this case, as well as the loop antenna  21  therebetween). The antennas  18 A and  18 B are preferably positioned outside of the metal body of the tool, and are thereby shielded from electromagnetic communication with regions of the borehole which lie behind the metal body or regions of other formations in directions intercepted by the metal body. As illustrated in FIG. 3, the antennas  18 A and  18 B each have a metal trough-shaped body  29  and an elongated center probe  42 , across which signals are applied. Each antenna effectively operates as a current loop which produces an oscillating RF magnetic field B 1  that is generally azimuthal in the volume of investigation and substantially perpendicular to the static magnetic field, B 0  (which is generally radial in the volume of investigation). The loop  21  has an axis that is generally radial (that is, perpendicular to the longitudinal axis of the logging device and the borehole), and is sensitive to radial signals. The trough-shaped body  29  has end plates  40 ,  41  with the center conductor or probe  42  extending from one end plate  40  to the other end plate  41 , parallel to and centered in the semi-cylindrical trough  29 . The U.S. Pat. No. 5,153,514 discloses that the trough antenna, which can be filled with a ferrite, can have an inner conductive shell that is separated from a steel body by a rubber layer, which suppresses magnetoacoustic ringing. It will be understood that various other types of magnetic resonance logging equipment can be used in practicing the invention, a further example being shown in FIG. 8 below. 
     FIG. 4 is a block diagram, partially in schematic form, of an embodiment of the downhole circuitry of logging device  30 . A downhole processor subsystem can conventionally include a processor  410  (e.g. any suitable microprocessor) with associated memory  413  and clock/timing circuitry  414 . Telemetry circuitry  490 , coupled with the processor subsystem, is conventionally provided for communication with the earth&#39;s surface. Transmitter circuitry  420 , under control of the processor subsystem, provides transmitter signals to RF antennas  18 A and  18 B. The transmitter circuitry can be of the general type disclosed in U.S. Pat. No. 5,055,787, and includes one or more oscillators and pulse formers which, in the present embodiment, are utilized in the generation of pulses of RF at the Larmor frequency in the volume of investigation (e.g., generally, region  9  in FIG. 1) for tipping the direction of the spins therein, preferably by 180 degrees. In the embodiment of FIG. 4, the pick-up loop antenna  21 , shown adjacent formations  31 , is part of an ambient temperature circuit that employs a SQUID.(Superconducting Quantum Intoferometric Device). [In the embodiment of FIG. 5, described subsequently, the pick-up antenna is in the cooled enclosure together with the SQUID.] In the FIG. 4 circuit, the pick-up coil  21  is coupled in a circuit having resistance  425  (the resistance of the wire, which is preferably minimized) and an input coil  430  of a SQUID  440 . The input coil and SQUID are in a cooled enclosure  435  that is cooled by a cooling unit  437  that may be, for example, a liquid nitrogen cooling unit. A current source  445  provides input current to the SQUID  440 , and the voltage across the SQUID, which is a measure of the sensed magnetic flux, is amplified by output amplifier  450 . The amplified signal is coupled to analog-to digital converter  425 , which samples under control of timing from processor  410  and whose output is, in turn, coupled to processor  410 . 
     In the embodiment of FIG. 5, the pick-up loop  21 A is in the cooled enclosure ( 435 A), together with the input loop  430 A and the SQUID  440 A. The enclosure can advantageously be a dewared all-metal enclosure. There is no resistance in the superconducting loop circuit. The output of amplifier  450  is then coupled to analog-to digital converter  455  (of FIG.  4 ). 
     In the embodiments of FIGS. 4 and 5, to cancel out time varying but spatially homogeneous fluxes, such as might be encountered by a tool moving in the earth&#39;s field, the pick-up loop can be a matched pair of loops connected in series opposition, with one loop being more sensitive to the formation than the other. 
     Referring to FIG. 6, there are shown graphs labeled  6 A,  6 B, and  6 C, each as a function of time, which are useful in understanding the signals produced and detected when using embodiments of the present invention. The graph  6 A represents the static magnetic field (assuming, for ease of illustration, that the logging device has moved into the investigation region at a time equals zero), the graph  6 B represents the applied RF tipping pulse, and the graph  6 C represents the magnetization (magnetic flux) sensed by the detection antenna  21  and associated circuitry. The graph  6 A illustrates the static magnetic field, B 0 , which, in the illustrated embodiments hereof, is produced by permanent magnets. In terms of a logging device moving through the borehole, the time t=0 can approximate the time that the logging device reaches a particular depth level at which the described logging measurements are to be made. After sufficient time for the spins in an investigation region to be polarized, an RF tipping pulse  615  is applied. For resonant operation, the RF is at the Larmor frequency of the spins (determined by the strength of the static magnetic field in the investigation region and the gyromagnetic ratio), and the duration of the pulse determines the tipping angle. In a preferred embodiment hereof, the tipping pulse is a 180 degree pulse. The graph  6 C shows the magnetic field strength (magnetic flux) that is seen by the antenna  21 . As the spins are initially polarized in the direction of the static field, the magnetic flux is seen to gradually build up (reference numeral  621 ). Then, the 180 degree RF pulse reverses the direction of magnetization of the spins, and thereby reverses the polarity of the magnetic field sensed by the detector, as seen at reference numeral  622  in the graph  6 C. Then, in the region of the plot designated by reference numeral  623 , the antenna  21  sees the magnetic field from of the spins as they gradually realign with the static field direction, with a characteristic longitudinal relaxation time constant T 1 . The equation for magnetization M that defines the curve  623  is: 
     
       
           M=M   0 (1−2 e   −t/T     1   ) 
       
     
     where M 0  is the magnetization of the polarized spins in the static field, and T 1  is the longitudinal relaxation time constant. It will be understood that for media having a distribution of T 1 &#39;s, the curve  623  will be a weighted sum of exponentials, with each exponential having a T 1  that is characteristic of the particular substance and a weighting coefficient that depends on the number of resonated spins in the particular substance. The points on the curve  623  (as illustrated generally in graph  6 A) are representative digitized points that are sampled and input to the processor subsystem of FIG. 4 by analog-to-digital converter  425 . The value of T 1  and/or the T 1  distribution can then be computed downhole, uphole, or at a remote location, using any suitable known technique, for example the type of technique disclosed in D. P. Gallegos and D. M. Smith, “A NMR Technique For The Analysis Of Pore Structure”, Journal Of Colloid And Interface Science, 122, 143-153 (1988). 
     As first noted above, the RF tipping pulse will preferably be a 180 degree tipping pulse that will cause the spins to reverse direction. This will provide the maximum signal excursion (2M 0 ) for determination of T 1 . However, it will be understood that operation can still be implemented if reversal is incomplete; that is for a tipping pulse of less or more than 180 degrees. [The tip angle depends on the RF pulse duration and magnitude. The rotation axis depends on the difference between the RF frequency and the Larmor frequency. Thus, a 180 degree tipping pulse for a given region of the formation will be a non-180 degree pulse in other formation regions where the magnitude of the static field is different.] The situation for a non-180 degree tipping angle, α, is shown in graphs  7 A,  7 B, and  7 C. The graph  7 A again illustrates the static magnetic field, the graph  7 B illustrates the RF tipping pulse (at, say, an angle α that is between 90 degrees and 180 degrees), and the graph  7 C illustrates the magnetic field strength (magnetic flux) that is seen by antenna  21 . In this case, if the field magnitude before tipping is again M 0 , the field magnitude, M, in the longitudinal direction (static field direction) after tipping will be 
     
       
           M=M   0 (cos α) 
       
     
     and the exponential curve  723  will be in accordance with 
     
       
           M=M   0 [1−(1−cos α) e   −t/T     1   ]. 
       
     
     As described so far, the magnetization of the spins is perturbed using an RF field with resonant operation, but it will be understood that alternative techniques can be employed. For example, if B 0  is changed (in either magnitude or direction), the magnetization will adjust to the new B 0  with the same time longitudinal relaxation time. For this general case we have 
       M=χB   0   
     where M (a vector) is the longitudinal nuclear magnetization, B 0  (a vector) is the applied magnetic field (from permanent magnets, current carrying coils, the earth, or a combination of those) and χ is the nuclear magnetic susceptibility. Thus, changing B 0  will change M, as shown in FIGS. 8A and 8B. If the time that the field is changed is t=0, then the equation for M (for the case of a single exponential decay) is 
     
       
           M=M   f +( M   i   −M   f )exp[− t/T   1   ]=χB   f +(χ B   i   −χB   f )exp[− t/T   1 ] 
       
     
     where the subscript i represents initial value and the subscript f represents final value. This magnetization change (which can be growth or decay) can be sensed in the same manner as if an RF pulse had been applied, as previously described. 
     The two transmitting antennas of the present embodiment can be used to advantage as follows: When the sonde is moving up the borehole, the upper antenna can be energized to tip the spins in front of it. As the sonde moves, it carries the receiving antenna into close proximity to the tipped spins, which are in the process of recovering to their equilibrium state along the static field direction. If the tool is only used to log up, the lower antenna can be dispensed with. On the other hand, if the tool is used to log while descending, the lower antenna would be the one to be energized. When the tool is stopped (or moving very slowly) both antennas can be energized. In such case, neither tips the spins in front of the receiver very efficiently, but the fringing RF fields from both have some effect. 
     FIG. 9 illustrates a further embodiment which utilizes a radial static field from opposing permanent magnets, as in J. Jackson, New NMR Well Logging/Fracture Mapping Technique With Possible Application Of SQUID NMR Detection, Soc. Of Explor. Geo., Tulsa, Okla., pp. 161-165, 1981. In this and other embodiments, the permanent magnets can be cooled (as in the reference). In the FIG. 9 embodiment, the logging device  930  has a body  940  that contains cylindric magnets  951 ,  952  of opposing polarity. The RF transmitting loop or coil  915  can be centrally located, as shown, in a recess in the logging device (or in a drill collar in a logging-while-drilling application). The axis of coil  915  is coincident with the tool axis and generally, with the borehole axis. One or more sensing loop antennas, each connected to a SQUID or another magnetic field flux detector, can be wound as a saddle coil (e.g. shown at  918 ) on the sonde so as to be sensitive to the changing radial magnetic field due to longitudinal nuclear spin relaxation. The apparatus may be rotating during the measurement if the measurement is made on a turning drill collar. In that case, an azimuthally resolved measurement can be made by correlating the instantaneous longitudinal magnetic signal with the rotation angle of the apparatus. 
     Existing superconductors will operate at or somewhat above liquid nitrogen temperature. In the absence of very large cooling powers it will be preferable to thermally shield the superconducting antenna with a vacuum dewar. This, in turn, necessitates the use of a metal structure that will not collapse under borehole pressure. For relatively low frequency measurements, such as those employed in the described embodiment, the pick-up loop can be located inside an all-metal enclosure such as a 0.25″ titanium pressure housing. The frequency at which the housing constitutes one skin depth is about 30 kHz. For higher frequency operation, a section of the housing having a reduced wall thickness can be used. The stress on this section can be computed (see Marks, Standard Handbook For Mechanical Engineers, 8th Edition, Chapter 5) as: 
     
       
         
           St=wr 
           2 
           /t 
           2 
         
       
     
     where w is the uniformly distributed load on a circular section, r is its radius, and t is its thickness. Taking w=20,000 psi and St=80,000 psi, which is the yield strength of titanium (see Marks, supra), then a ½″ diameter section should be ⅛″ thick. This is one skin depth at 130 kHz, and is appropriate for intermediate frequency measurements using superconducting sense coils. 
     The frequency selectivity of the metal housing which houses the receiver (but not the transmitter(s), which are outside the housing) is an advantage of embodiments of the invention. The frequency broadcast by the transmitting antenna(s) is at the Larmor frequency used to tip the spins, and is at a frequency (for example, 2 MHz) too high to penetrate metal housing walls of useful thickness. However, the magnetization decay of interest sensed by the receiver has a decay of the order of 0.1 msec or slower. A decay with a 0.1 msec time constant has spectral (Fourier) components in the frequency range between about 0 Hz and 10 kHz. For example, the 0.25 inch titanium pressure housing will easily pass the received signal, but not a 2 MHz transmitted pulse. Thus, since the receiver is completely shielded from the transmitted pulse, it will not be overloaded by the transmitted pulse. In contrast to existing NMR logging devices, there will be little or no receiver dead time, for example when operating the embodiment of FIG.  5 . 
     The SQUID used in embodiments hereof can preferably be made with high T c  superconductor, and can operate at or above the temperature of liquid nitrogen (77 K). Mechanical and thermophysical refrigerators are known which can maintain the cooled enclosure at temperatures needed to sustain superconductivity. Precooled thermal masses could also be employed.