GB1384099A - Pulsed neutron logging system with gain compensation - Google Patents
Pulsed neutron logging system with gain compensationInfo
- Publication number
- GB1384099A GB1384099A GB3946572A GB3946572A GB1384099A GB 1384099 A GB1384099 A GB 1384099A GB 3946572 A GB3946572 A GB 3946572A GB 3946572 A GB3946572 A GB 3946572A GB 1384099 A GB1384099 A GB 1384099A
- Authority
- GB
- United Kingdom
- Prior art keywords
- channel
- gain
- register
- amplifier
- sub
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 239000000523 sample Substances 0.000 abstract 3
- 239000013078 crystal Substances 0.000 abstract 2
- 238000001228 spectrum Methods 0.000 abstract 2
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 abstract 1
- 230000005251 gamma ray Effects 0.000 abstract 1
- 229910052739 hydrogen Inorganic materials 0.000 abstract 1
- 239000001257 hydrogen Substances 0.000 abstract 1
- 230000004048 modification Effects 0.000 abstract 1
- 238000012986 modification Methods 0.000 abstract 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V5/00—Prospecting or detecting by the use of ionising radiation, e.g. of natural or induced radioactivity
- G01V5/04—Prospecting or detecting by the use of ionising radiation, e.g. of natural or induced radioactivity specially adapted for well-logging
- G01V5/08—Prospecting or detecting by the use of ionising radiation, e.g. of natural or induced radioactivity specially adapted for well-logging using primary nuclear radiation sources or X-rays
- G01V5/10—Prospecting or detecting by the use of ionising radiation, e.g. of natural or induced radioactivity specially adapted for well-logging using primary nuclear radiation sources or X-rays using neutron sources
- G01V5/101—Prospecting or detecting by the use of ionising radiation, e.g. of natural or induced radioactivity specially adapted for well-logging using primary nuclear radiation sources or X-rays using neutron sources and detecting the secondary Y-rays produced in the surrounding layers of the bore hole
- G01V5/102—Prospecting or detecting by the use of ionising radiation, e.g. of natural or induced radioactivity specially adapted for well-logging using primary nuclear radiation sources or X-rays using neutron sources and detecting the secondary Y-rays produced in the surrounding layers of the bore hole the neutron source being of the pulsed type
Landscapes
- Physics & Mathematics (AREA)
- High Energy & Nuclear Physics (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- Geophysics (AREA)
- Measurement Of Radiation (AREA)
- Geophysics And Detection Of Objects (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
Abstract
1384099 Gain control in well logging systems TEXACO DEVELOPMENT CORP 24 Aug 1972 [20 Sept 1971] 39465/72 Heading G1A In a well logging system comprising a sub-surface probe containing a neutron source 16 and a scintillation crystal 12 with a photo-multiplier 11 for receiving the gamma rays from the areas surrounding the sub-surface probe 2 and wherein the height of the pulses emitted by the photo-multiplier 11 represents the energy of the gamma ray causing it, variations in the gain of the crystal or the photomultiplier are corrected by adjusting the gain of an amplifier 24 in dependence upon difference between the measured location of a peak in the spectrum from its known location. As shown the pulses from the sub-surface probe are amplified and fed into an integrator which holds a gate open for a duration depending on the magnitude of the pulse height and allows a high frequency oscillator 29 to supply a channel address register 30 so that at the end of the duration the register 30 has a binary number representing the pulse height. The circuit shown is such that each binary number (or range of numbers) is associated with a particular energy channel 31 and at any instant each channel contains a number representing the sum of the number of counts (or pulses) that have occurred with its associated energy value. The contents of three channel registers 2, 3, 4 are supplied to a signal comparator circuit 46, and initially one channel register 3 is chosen to coincide with a peak in the spectrum (i.e. the 2À23 MEV hydrogen peak) and the channel register generates a voltage signal on line 25 whose amplitude is proportional to the difference between the contents of channel register 3 and the contents of either channel register 2 or channel register 4 whichever difference is larger. Then if any gain drift occurs the signal comparator 46 will detect a change in the relative proportions and will generate an error signal of appropriate amplitude and sign. The error signal is fed back via line 25 to the control input of amplifier 24 of the pulse height analyser and will cause a change in the gain of the amplifier to compensate for the drift. In a modification a plurality of peaks are monitored providing a plurality of error signals which are fed via a logic circuit which controls the amplifier.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US18191071A | 1971-09-20 | 1971-09-20 |
Publications (1)
Publication Number | Publication Date |
---|---|
GB1384099A true GB1384099A (en) | 1975-02-19 |
Family
ID=22666321
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB3946572A Expired GB1384099A (en) | 1971-09-20 | 1972-08-24 | Pulsed neutron logging system with gain compensation |
Country Status (12)
Country | Link |
---|---|
JP (1) | JPS559670B2 (en) |
KR (1) | KR780000747B1 (en) |
AR (1) | AR213058A1 (en) |
AU (1) | AU457489B2 (en) |
BR (1) | BR7206468D0 (en) |
CA (1) | CA963178A (en) |
DE (1) | DE2245833C3 (en) |
DK (1) | DK139919B (en) |
ES (1) | ES406787A1 (en) |
FR (1) | FR2153322B1 (en) |
GB (1) | GB1384099A (en) |
MY (1) | MY7800306A (en) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS56110142U (en) * | 1980-01-28 | 1981-08-26 | ||
FR2485752A1 (en) * | 1980-06-25 | 1981-12-31 | Schlumberger Prospection | METHOD AND DEVICE FOR MEASURING GAMMA RAYS IN A SURVEY |
JPS59207400A (en) * | 1983-05-10 | 1984-11-24 | 株式会社彦間製作所 | Detecting mechanism of load of lifting gear |
-
1972
- 1972-08-24 GB GB3946572A patent/GB1384099A/en not_active Expired
- 1972-08-29 AU AU46076/72A patent/AU457489B2/en not_active Expired
- 1972-09-11 AR AR24401172A patent/AR213058A1/en active
- 1972-09-12 JP JP9098172A patent/JPS559670B2/ja not_active Expired
- 1972-09-12 KR KR7201378A patent/KR780000747B1/en active
- 1972-09-18 ES ES406787A patent/ES406787A1/en not_active Expired
- 1972-09-18 BR BR646872A patent/BR7206468D0/en unknown
- 1972-09-18 CA CA151,970A patent/CA963178A/en not_active Expired
- 1972-09-19 DE DE19722245833 patent/DE2245833C3/en not_active Expired
- 1972-09-20 FR FR7233246A patent/FR2153322B1/fr not_active Expired
- 1972-09-20 DK DK463972A patent/DK139919B/en unknown
-
1978
- 1978-12-30 MY MY7800306A patent/MY7800306A/en unknown
Also Published As
Publication number | Publication date |
---|---|
AU4607672A (en) | 1974-03-07 |
FR2153322B1 (en) | 1976-05-21 |
MY7800306A (en) | 1978-12-31 |
BR7206468D0 (en) | 1973-07-19 |
DE2245833B2 (en) | 1978-06-01 |
DE2245833A1 (en) | 1973-04-12 |
FR2153322A1 (en) | 1973-05-04 |
AR213058A1 (en) | 1978-12-15 |
DE2245833C3 (en) | 1979-01-25 |
JPS559670B2 (en) | 1980-03-11 |
ES406787A1 (en) | 1975-11-01 |
DK139919C (en) | 1979-10-15 |
CA963178A (en) | 1975-02-18 |
AU457489B2 (en) | 1975-01-30 |
DK139919B (en) | 1979-05-14 |
KR780000747B1 (en) | 1978-12-30 |
JPS4838801A (en) | 1973-06-07 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PS | Patent sealed | ||
PCNP | Patent ceased through non-payment of renewal fee |