EP1256018A1 - Verfahren und vorrichtung zur messung der ionisierenden stralungen mit hintergrundkorrectur - Google Patents
Verfahren und vorrichtung zur messung der ionisierenden stralungen mit hintergrundkorrecturInfo
- Publication number
- EP1256018A1 EP1256018A1 EP01907808A EP01907808A EP1256018A1 EP 1256018 A1 EP1256018 A1 EP 1256018A1 EP 01907808 A EP01907808 A EP 01907808A EP 01907808 A EP01907808 A EP 01907808A EP 1256018 A1 EP1256018 A1 EP 1256018A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- radiation
- measurement
- measuring
- detector
- source
- 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.)
- Withdrawn
Links
- 230000005855 radiation Effects 0.000 title claims abstract description 40
- 238000000034 method Methods 0.000 title claims abstract description 9
- 238000012937 correction Methods 0.000 title claims description 6
- 238000005259 measurement Methods 0.000 claims abstract description 59
- 230000005865 ionizing radiation Effects 0.000 claims description 11
- 230000000694 effects Effects 0.000 abstract description 9
- 238000001514 detection method Methods 0.000 description 9
- 230000006870 function Effects 0.000 description 3
- LPLLVINFLBSFRP-UHFFFAOYSA-N 2-methylamino-1-phenylpropan-1-one Chemical compound CNC(C)C(=O)C1=CC=CC=C1 LPLLVINFLBSFRP-UHFFFAOYSA-N 0.000 description 1
- 240000003023 Cosmos bipinnatus Species 0.000 description 1
- 235000005956 Cosmos caudatus Nutrition 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 230000002596 correlated effect Effects 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 230000002285 radioactive effect Effects 0.000 description 1
- 229910052704 radon Inorganic materials 0.000 description 1
- SYUHGPGVQRZVTB-UHFFFAOYSA-N radon atom Chemical compound [Rn] SYUHGPGVQRZVTB-UHFFFAOYSA-N 0.000 description 1
- 239000002689 soil Substances 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
- 239000002699 waste material Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/16—Measuring radiation intensity
- G01T1/167—Measuring radioactive content of objects, e.g. contamination
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T7/00—Details of radiation-measuring instruments
Definitions
- the field of this invention is the measurement of ionizing radiation emitted by a source, and here we are concerned with correcting the measurement by overcoming the influence of background noise.
- the term “detector” has a broad meaning and can be translated in reality by a set of several detection sets. Attempts have already been made to avoid the effect of the background noise produced by this surrounding radioactivity. It is therefore common for the main detector, responsible for measuring the radiation from the source, to be supplemented by an auxiliary detector specifically responsible for measuring background noise. When it detects background noise of a level deemed to be excessive, the measurement of the radiation from the source is not undertaken and we can wait for more favorable circumstances for the which, however, is not convenient.
- the auxiliary detector completely envelops the main detector and the source when it is present: it then measures the ambient radiation originating from all directions in a uniform manner, but it does not prevent part of the ambient radiation to cross it and reach the main detector, which further falsifies the measurement.
- This radiation can be transmitted directly or after having been diffused and affected by the Compton effect, that is to say supplied at a different energy, which makes it difficult to evaluate according to the part of the radiation that the auxiliary detector has stopped.
- auxiliary detector is also sensitive to radiation originating from the source, transmitted directly or after passing through the main detector, it can be understood that these correction calculations are difficult to apply and require a complicated electronic operating system (anti-Compton devices) .
- the object of the invention is therefore to correct the influence of background noise, in the particular case of ionizing radiation measurements where it is very difficult to distinguish the influence of the various origins of the radiation, by means of a set detection and a process each improved.
- the invention consists in correcting the measurements of the main detector, responsible for evaluating the radiation from the source, estimating the background noise it records and subtracting it from these measurements; it relates to a unit for measuring ionizing radiation, comprising a main detector responsible for measuring radiation emitted by a determined source and an auxiliary detector responsible for measuring ambient radiation, characterized in that it comprises means for correlating the measurements made by the two detectors and the correction of the measurements made by the primary detector as a function of the results of the correlation; as well as a method for measuring ionizing radiation, comprising a main measurement of a main radiation emitted by a determined source and an auxiliary measurement of ambient radiation, as well as corrections of the main measurement as a function of the auxiliary measurement, characterized in that the main measurement begins before bringing the source and is compared with the auxiliary measurement to obtain a correlation, and in that, when the source has been brought, the main measurement is corrected according to the correlation and simultaneous auxiliary measurement.
- Figure 1 is a schematic view of the detection assembly
- Figures 2 and 3 are graphs of raw and corrected measurements.
- the whole of the invention which in a particular form can constitute an assembly called a portal for detection in specialized language, is in this case intended primarily to measure the activity of radioactive objects of various natures which pass in front of it. It comprises at least one main detector or measurement detector 1 responsible for measuring the activity of an irradiating source, and at least one auxiliary detector or guard detector 2 responsible for measuring the ambient radiation responsible for the background noise.
- Detectors 1 and 2 can be placed side by side at a greater or lesser distance from each other, or possibly, what is shown here, on either side of a location 3 occupied the source S.
- the source S is any object, of undetermined size and often of low activity in practice, such as the loading of a truck, a concrete block, a barrel of waste, etc.
- Detectors 1 and 2 which are only shown here, conventionally include a number of radiation detectors which receive ionizing radiation and convert it into electrical signals.
- the measurement detector 1 is of course sensitive to radiation from location 3, while the guard detector 2 can be made sensitive to radiation from all directions except location 3, from which it is separated by a shielding 4. These conditions are general enough for a large number of arrangements of detectors 1 and 2 to be possible.
- the application of the invention is not limited to gamma radiation, but is also possible for other types of radiation: alpha, beta, and X, in particular configurations of the main detector and the auxiliary detector.
- the work required of the detection unit generally includes relatively short measurement periods separated by much longer periods of inactivity and which can reach several hours. However, these periods of inactivity are used to make measurements of ambient radioactivity.
- the measured values alo-r-s by the two detectors 1 and 2 are recorded separately and compared.
- the inventors made the important observation that the measurements were correlated with one another and could therefore be deduced from each other by a regression operation.
- the counters 5 and 6 to which the detectors 1 and 2 are respectively connected and which serve to simultaneously record their measurements are read by a computer 7 which calculates the coefficients of the correlation curve, which in practice is sufficiently approximated by a straight line.
- the guard detector 2 continues to measure the ambient radiation.
- the computer 7 deduces therefrom the effect of this radiation on the measurement detector 1, that is to say the intensity of the background noise which it must restore and subtracts it from the total provided by the counter 5 to obtain the value of the radiation from source S. The results currently obtained have demonstrated the validity of the process.
- FIG. 2 shows, in addition to the corap-tage rates g and m for acquisition periods T of 10 min, measurements m X ⁇ , m x and m x3 carried out in a measurement period P3 with three successive sources.
- Line L is the detection limit, below which it is estimated that radiation can no longer be measured properly: “reduced” noise is still below this limit and the results appear suitable even for the third source, whose activity is barely above this limit.
- the invention does not only facilitate the detection of radiation, but also its measurement; it can therefore be applied to devices other than detection gates.
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- High Energy & Nuclear Physics (AREA)
- Molecular Biology (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Measurement Of Radiation (AREA)
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR0001900 | 2000-02-16 | ||
FR0001900A FR2805048B1 (fr) | 2000-02-16 | 2000-02-16 | Ensemble et procede de mesure de rayonnement ionisant avec correction de bruit de fond |
PCT/FR2001/000448 WO2001061378A1 (fr) | 2000-02-16 | 2001-02-15 | Ensemble et procede de mesure de rayonnement ionisant avec correction de bruit de fond |
Publications (1)
Publication Number | Publication Date |
---|---|
EP1256018A1 true EP1256018A1 (de) | 2002-11-13 |
Family
ID=8847043
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP01907808A Withdrawn EP1256018A1 (de) | 2000-02-16 | 2001-02-15 | Verfahren und vorrichtung zur messung der ionisierenden stralungen mit hintergrundkorrectur |
Country Status (4)
Country | Link |
---|---|
US (1) | US20030004406A1 (de) |
EP (1) | EP1256018A1 (de) |
FR (1) | FR2805048B1 (de) |
WO (1) | WO2001061378A1 (de) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2938927B1 (fr) * | 2008-11-27 | 2011-01-07 | Saphymo | Dispositif autonome et procede de controle de la contamination radioactive d'un utilisateur. |
WO2013067637A1 (en) | 2011-10-27 | 2013-05-16 | Atomic Energy Of Canada Limited/ Énergie Atomique Du Canada Limitée | Portable detection apparatus and method |
FR3011340B1 (fr) * | 2013-10-01 | 2017-01-06 | Commissariat Energie Atomique | Systeme de mesure de la radioactivite dans un bruit de fond gamma |
FR3086764B1 (fr) * | 2018-09-27 | 2020-12-25 | Commissariat Energie Atomique | Systeme de spectrometrie, procede de spectrometrie et produit programme d'ordinateur associes |
Family Cites Families (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3701902A (en) * | 1971-06-09 | 1972-10-31 | Dresser Ind | Dual detector compensated density wall logging system |
US3732422A (en) * | 1972-05-23 | 1973-05-08 | Atomic Energy Commission | Counter for radiation monitoring |
US3825760A (en) * | 1973-03-21 | 1974-07-23 | Nasa | Flame detector operable in presence of proton radiation |
US4404973A (en) * | 1981-04-20 | 1983-09-20 | Jack Lancaster | Heart muscle evaluation method and apparatus |
US4616137A (en) * | 1985-01-04 | 1986-10-07 | The United States Of America As Represented By The United States Department Of Energy | Optical emission line monitor with background observation and cancellation |
JPS61205886A (ja) * | 1985-03-08 | 1986-09-12 | Mitsubishi Heavy Ind Ltd | 放射線量検出方法 |
US5473162A (en) * | 1987-10-26 | 1995-12-05 | Baylor University | Infrared emission detection of a gas |
US4896965A (en) * | 1988-09-14 | 1990-01-30 | The United States Of America As Represented By The United States Department Of Energy | Real-time alkali monitoring system |
US5324948A (en) * | 1992-10-27 | 1994-06-28 | The United States Of America As Represented By The United States Department Of Energy | Autonomous mobile robot for radiologic surveys |
US6111511A (en) * | 1998-01-20 | 2000-08-29 | Purdue Research Foundations | Flame and smoke detector |
-
2000
- 2000-02-16 FR FR0001900A patent/FR2805048B1/fr not_active Expired - Fee Related
-
2001
- 2001-02-15 EP EP01907808A patent/EP1256018A1/de not_active Withdrawn
- 2001-02-15 US US10/182,782 patent/US20030004406A1/en not_active Abandoned
- 2001-02-15 WO PCT/FR2001/000448 patent/WO2001061378A1/fr not_active Application Discontinuation
Non-Patent Citations (1)
Title |
---|
See references of WO0161378A1 * |
Also Published As
Publication number | Publication date |
---|---|
FR2805048A1 (fr) | 2001-08-17 |
FR2805048B1 (fr) | 2002-05-03 |
US20030004406A1 (en) | 2003-01-02 |
WO2001061378A1 (fr) | 2001-08-23 |
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Legal Events
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18D | Application deemed to be withdrawn |
Effective date: 20070901 |