Borehole measurements using a fast and high energy resolution gamma ray detector assembly
View Patent ↗A 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 and a digital spectrometer that cooperates with the crystal to maximize pulse processing throughput by digital filtering and digital pile-up inspection of the pulses. The detector assembly is capable of digital pulse measurement and digital pile-up inspection with dead-time less than 600 nanoseconds per event. Pulse height can be accurately measured (corrected for pile-up effects) for 2 pulses separated by as little as 150 nanoseconds. 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 carbon/oxygen logging.
1. A borehole instrument comprising a neutron generator axially spaced from a gamma ray detector assembly, said assembly comprising:
a LaBr3 scintillation crystal; and
a digital spectrometer cooperating with said LaBr 3 scintillation crystal and configured to
measure pulses from said scintillation crystal,
digitally filter said pulses from said scintillation crystal,
digitally inspect the filtered pulses to detect pile-up pulses,
periodically forming an estimate of an average ratio of said measured pulses per non-pile-up pulse, and
reject said pile-up pulses by combining said measured pulses with said ratio;
wherein;
said neutron generator emits a plurality of bursts of neutrons the duration of each burst of said plurality of bursts being about 30 microseconds and said plurality of bursts being emitted at a repetition rate of about 5 KHz; and
said detector assembly is operated during said bursts.
2. The borehole instrument of claim 1 wherein said detector assembly measures pulses and digitally filters pulses and digitally inspects pulses and rejects said pile-up pulses with dead-time less than 600 nanoseconds per event.
3. The borehole instrument of claim 1 wherein said detector assembly measures and resolves heights of two said pulses separated by about 150 nanoseconds.
4. The borehole instrument of claim 1 wherein said detector assembly operates at about 325 degrees Fahrenheit.
5. The borehole instrument of claim 1 wherein said borehole instrument is conveyed by a wireline or a drill string or coiled tubing or a slick line or drilling fluid flow.
6. The borehole instrument of claim 1 wherein a first group said pulses is collected in a gamma ray energy range of about 3.0 MeV to about 4.7 MeV and a second group is collected in a gamma ray energy range of about 4.7 MeV to about 6.4 MeV.
7. A borehole instrument comprising a neutron generator axially spaced from a gamma ray detector assembly, said assembly comprising:
a LaBr3 scintillation crystal; and
a digital spectrometer cooperating with said LaBr3 scintillation crystal and configured to
measure pulses from said scintillation crystal,
digitally filter said pulses from said scintillation crystal,
digitally inspect the filtered pulses to detect pile-up pulses, and
reject said pile-up pulses;
wherein
said neutron generator emits a plurality of bursts of neutrons the duration of each burst of said plurality of bursts being about 30 microseconds and said plurality of bursts being emitted at a repetition rate of about 5 KHz; and said detector assembly is operated during said bursts;
a first group said pulses is collected in a gamma ray energy range of about 3.0 MeV to about 4.7 MeV and a second group is collected in a gamma ray energy range of about 4.7 MeV to about 6.4 MeV;
a C/O ratio is formed from the ratio of said first group to said second group;
said C/O ratio is indicative of the amount of carbon to oxygen within environs in which said borehole instrument operates; and
determining said C/O ratio to a precision of about 0.012 standard deviation for a 20 second sample for a single detector.
8. The borehole instrument of claim 7 wherein said detector assembly measures pulses and digitally filters pulses and digitally inspects pulses and rejects said pile-up pulses with dead-time less than 600 nanoseconds per event.
9. The borehole instrument of claim 7 wherein said detector assembly measures and resolves heights of two said pulses separated by about 150 nanoseconds.
10. The borehole instrument of claim 7 wherein said detector assembly operates at about 325 degrees Fahrenheit.
11. The borehole instrument of claim 7 wherein said borehole instrument is conveyed by a wireline or a drill string or coiled tubing or a slick line or drilling fluid flow.
12. A method for measuring radiation in a borehole, the method comprising:
disposing a gamma ray detector assembly within said borehole wherein said assembly comprises a LaBr 3 scintillation crystal; and a digital spectrometer cooperating with said LaBr3 scintillation crystal and configured to measure pulses from said scintillation crystal, digitally filter said pulses from said scintillation crystal, digitally inspect the filtered pulses to detect pile-up pulses, periodically forming an estimate of an average ratio of said measured pulses per non-pile up pulse, and reject said pile-up pulses by combining said measure of pulses with said ratio;
disposing a neutron generator within said borehole axially spaced from the detector assembly;
generating a plurality of bursts of neutrons with the neutron generator wherein the duration of each said burst is about 30 microseconds and said plurality of bursts is emitted at a repetition rate of about 5 KHz; and
operating the detector assembly during each burst of said plurality of bursts.
13. The method of claim 12 further comprising, with said detector assembly, measuring and digitally filtering and digitally inspecting and rejecting said pile-up pulses with dead-time less than 600 nanoseconds.
14. The method of claim 12 further comprising, with said detector assembly, accurately measuring heights of two said pulses separated by about 150 nanoseconds.
15. The method of claim 12 further comprising operating said detector assembly at about 325 degrees Fahrenheit.
16. The method of claim 12 wherein:
said detector assembly and said neutron generator are disposed within a borehole instrument that is conveyed in said borehole by a wireline or a drill string or coiled tubing or a slick line or drilling fluid flow.
17. The method of claim 12 further comprising collecting a first group said pulses in a gamma ray energy range of about 3.0 MeV to about 4.7 Mev and collecting a second group of said pulses in a gamma ray energy range of about 4.7 MeV to about 6.4 MeV.
18. A method for measuring radiation in a borehole, the method comprising:
disposing a gamma ray detector assembly within said borehole wherein said assembly comprises a LaBr 3 scintillation crystal; and a digital spectrometer cooperating with said LaBr3 scintillation crystal and configured to measure pulses from said scintillation crystal, digitally filter said pulses from said scintillation crystal, digitally inspect the filtered pulses to detect pile-up pulses, and reject said pile-up pulses;
disposing a neutron generator within said borehole axially spaced from the detector assembly;
generating a plurality of bursts of neutrons with the neutron generator wherein the duration of each said burst is about 30 microseconds and said plurality of bursts is emitted at a repetition rate of about 5 KHz;
operating the detector assembly during each burst of said plurality of bursts;
collecting a first group said pulses in a gamma ray energy range of about 3.0 MeV to about 4.7 MeV and collecting a second group of said pulses in a gamma ray energy range of about 4.7 MeV to about 6.4 MeV;
forming a C/O ratio from a ratio of said first group to said second group;
from said C/O ratio determining an indicator of the amount of carbon to oxygen within environs in which said borehole instrument is operating; and
determining said C/O ratio to a precision of about 0.012 standard deviation for a 20 second sample for a single detector.
19. The method of claim 18 further comprising, with said detector assembly, measuring and digitally filtering and digitally inspecting and rejecting said pile-up pulses with dead-time less than 600 nanoseconds.
20. The method of claim 18 further comprising, with said detector assembly, accurately measuring heights of two said pulses separated by about 150 nanoseconds.
21. The method of claim 18 further comprising operating said detector assembly at about 325 degrees Fahrenheit.
22. The method of claim 18 wherein:
said detector assembly and said neutron generator are disposed within a borehole instrument that is conveyed in said borehole by a wireline or a drill string or coiled tubing or a slick line or drilling fluid flow.
23. The method of claim 18 further comprising collecting a first group said pulses in a gamma ray energy range of about 3.0 MeV to about 4.7 MeV and collecting a second group of said pulses in a gamma ray energy range of about 4.7 MeV to about 6.4 MeV.