This application is a reissue application of U.S. Pat. No. 7,999,220, which was derived from U.S. patent application Ser. No. 12/129,812, filed on May 30, 2008, which is herein incorporated by reference in its entirety for all purposes.
Borehole well logging systems that emit bursts of high energy (of the order of 14 million electron volts (MeV)) neutrons are routinely used in geophysical exploration, recovery and monitoring operations. These systems are typically used in cased boreholes, although some uncased or “open hole” applications are known in the art. As examples, pulsed neutron logging systems are used to measure formation density in cased boreholes, to determine formation lithology, to detect gas within formation pore space, and to identify and to optionally measure the flow of water behind casing.
The earliest commercial pulsed neutron logging system was to delineate saline formation liquid from non-saline liquid, which was assumed to be liquid hydrocarbon. Chlorine in saline water has a relatively large thermal neutron absorption cross section, while carbon and hydrogen in hydrocarbons have relatively small thermal neutron cross sections. The decay rate of thermal neutrons is measured between bursts of fast neutrons by measuring capture gamma radiation as a function of time. This decay rate is, therefore, indicative of the thermal neutron capture cross section of the borehole environs. This quantity is commonly referred to as “sigma”. Based upon the large difference thermal neutron absorption cross section of saline water and liquid hydrocarbon, sigma combined with other measurements such as formation porosity is used to obtain a hydrocarbon saturation value for the formation. Again, this saturation value is based upon the assumption that any non-saline pore fluid is hydrocarbon.
All formation waters are not saline. A measure of sigma cannot, therefore, be used to delineate unequivocally between fresh formation water and liquid hydrocarbon. The “carbon/oxygen” or “C/O” logging system was developed to delineate between fresh water and hydrocarbon. The methodology of the C/O logging system is based upon a measure of a ratio of carbon to oxygen content of the borehole environs. This ratio can be used to delineate between fresh formation water and liquid hydrocarbon, because hydrocarbon contains carbon but no oxygen, and fresh water contains oxygen but no carbon. The system, like its “sigma” logging system counterpart, uses a pulsed source of 14 MeV neutrons. The system uses a measure of inelastic scatter gamma radiation (rather than thermal capture gamma radiation) to obtain desired results. Inelastic scatter cross sections are sufficiently large, and the emitted inelastic scatter radiation is sufficiently different in energy to permit the measure of an inelastic gamma radiation ratio indicative of the C/O ratio of the borehole environs. Inelastic scatter reactions are many orders of magnitude faster than the thermal capture process used in sigma logging. As a result, the inelastic scatter radiation measurement must be made during the neutron burst. This results in a very intense “instantaneous” gamma radiation field at the detector assembly. The received radiation is amplified as pulses of collected light and the height of the pulse is related to incident gamma-ray energy. Accurate measurement of the pulse height is corrupted by pulse pile-up (i.e. where one pulse is superimposed on another) resulting from the intense instantaneous radiation. The rejection of pile-up events yields a very low “observed” inelastic count rate from which the C/O information is derived. Stated another way, the observed statistical precision of C/O logging is typically poor even though the “instantaneous” inelastic scatter radiation flux during the burst is quite large. It is of the utmost importance, therefor, to use a fast gamma ray detection system and to minimize pulse pile-up during a measure interval to maximize the statistical precision and the accuracy of measured radiation attributable to carbon and to oxygen inelastic scattering.
The invention is directed to gamma ray detector assembly for a borehole logging system that requires the measure of gamma radiation with optimized gamma ray energy resolution and with fast emission times required to obtain meaningful measurements in high radiation fields. The detector assembly comprises a lanthanum bromide (LaBr3) scintillation crystal that exhibits outstanding peak resolution and emission time compared to other types of scintillation crystals. For carbon/oxygen logging, another advantage of LaBr3 and other higher density halides such as LaI (U.S. Pat. No. 7,084,403) and LuI (U.S. Pat. No. 7,329,874), is that the lack of oxygen in the crystal matrix offers an incremental boost in C/O sensitivity per unit volume, compared to fast, higher density detectors such as LYSO, GSO, LUAP that contain oxygen.
In intense gamma radiation fields, speed of detector pulse processing and pulse throughput are important considering the discussion in the BACKGROUND section of this disclosure. To maximize processing throughput and to maintain high resolution requires fast measurement and pile-up inspection of the pulses. A digital spectrometer has been designed based on digital filtering and digital pulse pile-up inspection that offers speed and energy resolution improvements over traditiontraditional analog measurement and inspection techniques. Concepts of this digital spectrometer are disclosed in U.S. Pat. No. 6,590,957 B1, which is here in entered into this disclosure by reference. The topology of the system in the referenced disclosure has been redesigned and configured for high-temperature operations with a LaBr3 detector crystal for use in well logging. In practice, the detector assembly comprising the digital spectrometer and the LaBr3 crystal is limited by filtering of electronics noise and digital sampling rates. The detector assembly is capable of pulse measurement and digital pile-up inspection with dead-time less than 600 nanoseconds per detection event (nS/event). Pulse height (thus energy resolution) can be accurately measured (corrected for pile-up effects) for 2 pulses separated by as little as 150 nanoseconds (nS). This detector assembly performance is facilitated by the combination of the LaBr3 detector crystal and the digital filtering and digital pile-up inspection spectrometer of the referenced disclosure.
Although the invention is applicable to virtually any borehole logging methodology that uses the measure of gamma radiation in harsh borehole conditions, the invention is particularly applicable to C/O logging.
The manner in which the above recited features and advantages, briefly summarized above, are obtained can be understood in detail by reference to the embodiments illustrated in the appended drawings.
The invention will be disclosed as a multipurpose well logging system that is adaptable to measure previously mentioned geophysical logging applications. It should be understood that the invention could be equally embodied as a “stand-alone” system designed to measure a single parameter of interest such as a carbon/oxygen ratio.
The multipurpose pulsed-neutron system must be versatile enough to cover many different cased-hole applications including reservoir evaluation using sigma measurements, reservoir evaluation using carbon/oxygen (C/O) measurements, and behind casing water flow. The system must further providingprovide an alternative to traditional open-hole logging such as through casing density and neutron porosity logging, and gas detection. As a result, various design trade-offs are used in optimizing these specific applications. For example, the formation porosity is a measure of the spatial distribution of radiation and requires certain axial detector assembly spacings from the source. Carbon/oxygen (C/O) logging is a spectral energy measurement and requires high count-rates at detector assemblies axially spaced close to the neutron source.
The subsection 11 is operationally connected to an instrument subsection 24. The instrument subsection houses control circuits and power circuits to operate and control the elements of the subsection 11. A telemetry subsection 26 is operationally connected to the instrument section 24. A suitable connector 28 connects the multipurpose logging tool 10 to a lower end of a preferably multiconductor logging cable 30. The upper end of the logging cable 30 terminates at a draw works, which is well known in the art and is represented conceptually at 34.
Still referring to
Again referring to
Although shown embodied in a wireline logging tool, the detector assembly 11 can also be embodied in other borehole instruments. These instruments include pump-down (“memory”) instruments conveyed by drilling fluid flow, instruments conveyed by coiled tubing, instruments conveyed by a drill string, and instruments conveyed by a “slick line”.
The LaBr3 Detector Crystal
In 2006 the LaBr3(Ce) crystal was introduced in a logging package by Saint Gobain (www.saint-gobain.com) under the trademark BriLanCe380™. In Table 1, the physical parameters for this crystal are compared with properties of other scintillation crystals used in prior art well logging detector assemblies. The scintillation crystals are NaI, BGO, GSO in addition to LaBr3. The crystal properties are light output in percent, energy resolution in percent, crystal density in grams per cubic centimeter, effective atomic number, and scintillation decay time or “emission time” in microseconds.
Again referring to Table 1, the outstanding features of LaBr3 are the peak resolution, temperature response and emission time. In the gamma radiation energy ranges or “windows” used in one C/O logging method, good peak resolution is important to assure accurate energy calibrations. More advanced C/O logging methods use spectral fitting techniques such as Library Least Squares for formation lithology identification or C/O determination. This approach exploits the good energy resolution of LaBr3 to add more uniqueness to library spectrum elements. The temperature response assures good resolution and stable measurement across the temperature range encountered in the borehole environment.
Similar to NaI, LaBr3 exhibits a thermal neutron activation background. More specifically, the bromine in LaBr3 has a relatively large thermal neutron activation cross section with the induced isotopes being gamma ray emitters. Preliminary test results indicate that the bromine activation that appears on the tail of the decay is about twice as strong as the iodine activation in NaI. There are two activation daughters. The first is 82Br that decays with a half life of 1.47 days. The second and more troublesome is 80Br which has two decay modes with half lives of 17.68 minutes and 4.4 hours. This neutron activation background signal can be minimized by thermal neutron shielding of the LaBr3 crystal.
The Digital Spectrometer and Pulse Selection System
To achieve the optimal scintillation pulse throughput for the detector assembly, the detector assembly uses a digital spectrometer designed by XIA LLC that is disclosed in detail in the previously referenced U.S. Pat. No. 6,590,957 B1. The digital spectrometer has been configured to obtain detector assembly specifications discussed in subsequent sections of this disclosure.
Referring again to
Results Using the Detector Assembly
In practice, the response of the detector assembly 45 is limited by filtering of electronics noise and digital sampling rates. It has been demonstrated that the assembly 45 is capable of pulse measurement and pile-up inspection with dead-time of less than 600 nS/event. Pulse height can be accurately resolved and measured (corrected for pile-up pulse effects) for 2 pulses separated by as little as 150 nS.
It is instructive to express specifications of the LaBr3 crystal 46 cooperating with the digital spectrometer 49 in terms of well logging precision. In the context of C/O logging precision, the logging tool 10 was operated in high-porosity carbonate calibration standards with oil and water in the pore space and fresh water in the borehole. The neutron source was operated at a pulse repetition rate of about 5 kiloHertz (KHz) with each burst having a duration of about 30 microseconds. The “window ratio” C/O technique was used. Count rates refer to those recorded by the near detector assembly 16. The carbon count rate C represents first group of pulses recorded in the carbon energy window ranging from about 3.0 to about 4.7 MeV. The oxygen count rate O represents a second group of pulses recorded in the oxygen energy window ranging from about 4.7 MeV to about 6.4 MeV. A typical two foot (0.61 meters) logging sample at 6 feet (1.82 meters) per minute represents 20 seconds. Operating at 80 percent of the maximum throughput, the counts collected by the digital spectrometer 49 are approximately 52,000 and 30,000 for the carbon and oxygen windows, respectively. Given the C/O ratio for the standard with fresh water in the pore space is 1.73, the following expression for the standard deviation of the C/O ratio in this carbonate as:
The deviation of the C/O ratio is 0.012, and enfolding the dynamic range between these standards, the deviation is 7.7 saturation units (s.u.), which is an apparent improvement over prior art assemblies.
The above disclosure is to be regarded as illustrative and not restrictive, and the invention is limited only by the claims that follow.
Number | Name | Date | Kind |
---|---|---|---|
3747001 | Fasching et al. | Jul 1973 | A |
4476384 | Westphal | Oct 1984 | A |
4503328 | Neufeld | Mar 1985 | A |
4507554 | Hertzog et al. | Mar 1985 | A |
4766543 | Schmidt | Aug 1988 | A |
4872507 | Ronco et al. | Oct 1989 | A |
4937446 | McKeon et al. | Jun 1990 | A |
5025151 | Melcher | Jun 1991 | A |
5055676 | Roscoe et al. | Oct 1991 | A |
6590957 | Warburton et al. | Jul 2003 | B1 |
7067816 | Dorenbos | Jun 2006 | B2 |
7084403 | Srivastava | Aug 2006 | B2 |
7102125 | Samworth | Sep 2006 | B2 |
7383142 | Scoullar | Jun 2008 | B2 |
7439515 | Bak | Oct 2008 | B2 |
7541589 | Srivastava | Jun 2009 | B2 |
7573026 | Kurkoski | Aug 2009 | B2 |
7880134 | Kirkwood et al. | Feb 2011 | B2 |
8431885 | Roscoe | Apr 2013 | B2 |
20030076914 | Tiller | Apr 2003 | A1 |
20040149917 | Dorenbos et al. | Aug 2004 | A1 |
20050056774 | Samworth | Mar 2005 | A1 |
Number | Date | Country |
---|---|---|
2006029475 | Feb 2006 | WO |
Entry |
---|
“BrilLanCe 380 Scintillator—The Downhole advantage” Advertising Material. Saint Gobain Ceramics & Plastics. Dec. 2007. 4 pgs. |
Iltis, Alain, et al. “Lanthanum halide scintillators: Properties and applications” Nuclear Instruments and Methods in Physics Research A 563 (2006) pp. 359-363. |
Kernan, WJ. “Self-Activity in Lanthanum Halides” IEEE Nuclear Science Symposium Conference Record, vol. 2 (2002) pp. 1002-1005. |
Menge, Peter R., et al. “Performance of large lanthanum bromide scintillators” Nuclear Instruments and Methods in Physics Research A 579 (2007) pp. 6-10. |
Odom, RC, et al. “Experiments on Closely Spaced Detector Candidates for Carbon/Oxygen Logging” SPWLA 45th Annual Logging Symposium (Jun. 2004) pp. 1-14. |
Odom, RC, et al. “Experiments on Closely Spaced Detector Candidates for Carbon/Oxygen Logging” Petrophysics, vol. 46, No. 3 (Jun. 2005) pp. 188-198. |
Odom, RC, et al. “Design and Initial Field-Test Results of a New Pulsed Neutron Logging System for Cased Reservoir Characterization” SPWLA 49th Annual Logging Symposium (May 25-28, 2008) pp. 1-9. |
Roscoe, BA & Grau, JA. “Response of the Carbon/Oxygen Measurement for an Inelastic Gamma Ray Spectroscopy Tool” SPE 14460 Formation Evaluation (Mar. 1988) pp. 76-80. |
Roscoe, BA, et al. “A New Through-Tubing Oil-Saturation Measurement System” SPE 21413 (Nov. 1991) pp. 659-663. |
Walker et al. “Chart of the Nuclides” General Electric (1997) pp. 1-26. |
Westaway, P, et al. “Neutron-Induced Gamma Ray Spectroscopy for Reservoir Analysis” Society of Petroleum Engineer's Journal (Jun. 1983) pp. 553-564. |
Odom, Richard C., Improvements in a Through-Casing Pulsed-Neutron Density Log, SPE71742, pp. 1-9, 2001 SPE Annual Technical Conference and Exhibition, New Orleans, Louisiana Sep. 30, 2001. |
International Search Report from United Kingdom patent application No. GB090246.1 dated Sep. 23, 2009. |
Number | Date | Country | |
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Parent | 12129812 | May 2008 | US |
Child | 13967230 | US |