CN106290429B - A kind of PGNAA characteristic gamma rays power spectrum backoff algorithm - Google Patents

A kind of PGNAA characteristic gamma rays power spectrum backoff algorithm Download PDF

Info

Publication number
CN106290429B
CN106290429B CN201610886933.4A CN201610886933A CN106290429B CN 106290429 B CN106290429 B CN 106290429B CN 201610886933 A CN201610886933 A CN 201610886933A CN 106290429 B CN106290429 B CN 106290429B
Authority
CN
China
Prior art keywords
power spectrum
pgnaa
gamma ray
characteristic gamma
characteristic
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 - Fee Related
Application number
CN201610886933.4A
Other languages
Chinese (zh)
Other versions
CN106290429A (en
Inventor
赵龙
陆景彬
许旭
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Jilin University
Original Assignee
Jilin University
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Jilin University filed Critical Jilin University
Priority to CN201610886933.4A priority Critical patent/CN106290429B/en
Publication of CN106290429A publication Critical patent/CN106290429A/en
Application granted granted Critical
Publication of CN106290429B publication Critical patent/CN106290429B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N23/00Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
    • G01N23/20Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by using diffraction of the radiation by the materials, e.g. for investigating crystal structure; by using scattering of the radiation by the materials, e.g. for investigating non-crystalline materials; by using reflection of the radiation by the materials
    • G01N23/207Diffractometry using detectors, e.g. using a probe in a central position and one or more displaceable detectors in circumferential positions
    • G01N23/2076Diffractometry using detectors, e.g. using a probe in a central position and one or more displaceable detectors in circumferential positions for spectrometry, i.e. using an analysing crystal, e.g. for measuring X-ray fluorescence spectrum of a sample with wavelength-dispersion, i.e. WDXFS

Abstract

The invention discloses a kind of PGNAA equipment characteristic gamma ray power spectrum backoff algorithms.The principle of the algorithm is the proportionality constant k by the way that measured matter is calculatedEi(i=1~1024), by the band information carrying N, the airborne signals N0 that are mounted on the ionisation chamber (6) on PGNAA equipment (1) subsequent controlled nucleon operated belt conveyor scale, operation is compensated to characteristic gamma ray power spectrum, solves the power spectrum distortion phenomenon caused by tested material own absorption characteristic gamma ray.For PGNAA equipment characteristic gamma ray during penetrating tested material arrival gamma-ray detector, part gamma ray can have the phenomenon that distortion by tested material own absorption, finally obtained characteristic gamma ray power spectrum.

Description

A kind of PGNAA characteristic gamma rays power spectrum backoff algorithm
Technical field:
The present invention relates to a kind of power spectrum backoff algorithm, specifically a kind of PGNAA characteristic gamma rays power spectrum backoff algorithm.
Background technology:
Wink hair gamma neutron activation analysis technique (PGNAA) is a kind of quick, contactless multielement analysis technology, is being built The industries such as material, coal, thermoelectricity, metallurgy, mine have obtained a large amount of application.Wink hair gamma neutron activation analysis technique principle be With thermal neutron capture reaction occurs for tested material, generates characteristic gamma ray, and characteristic gamma ray passes through tested material to reach gal Horse ray detector forms core pulse signal, and core pulse signal is transformed into digital signal by multiple tracks processor, ultimately forms spy Levy gamma ray spectroscopy.Characteristic gamma ray while penetrating tested material, part ray can by tested material own absorption, Cause final characteristic gamma ray power spectrum that cannot represent true characteristic gamma ray power spectrum, when tested material total amount becomes When change, the attenuation of characteristic gamma ray can also change, and finally obtained gamma ray spectroscopy will have distortion phenomenon.
Invention content:
To solve characteristic gamma ray power spectrum problem of dtmf distortion DTMF, the present invention installs a nucleon additional after PGNAA equipment as shown in Figure 1 Belt conveyer scale, controlled nucleon operated belt conveyor scale by137Cs radioactive sources and ionisation chamber two parts are constituted, and the signal of ionisation chamber sends PGNAA equipment meters to Calculate host.
Theoretically the tested material characteristic gamma ray that more multiphonon activation generates is also more, but due to material itself Also there is attenuation, the characteristic gamma ray that detector is collected into can also decline with the e index that is added to of material gamma ray Subtract:
IEi=I0Ei×exp(-μmEitm) (1)
IO in formula0iIt represents and generates energy as the intensity of the characteristic gamma ray of Ei, IEiEnergy is represented after material as Ei Gamma ray intensity, μmEiExpression energy is mass attentuation coefficient of the characteristic gamma ray of Ei in material, with substance Atomic number and ray energy are related, tmFor the mass thickness of material.By formula 1 it is found that if it is known that μmEiAnd tmIt can measure Change Expressive Features gamma ray attenuation degree, to mathematically into be about to measure characteristic gamma ray amount be reduced to true spy Levy the compensation operation of gamma ray amount.
The present invention is mounted with a controlled nucleon operated belt conveyor scale after PGNAA equipment, uses137Cs radioactive sources, ionisation chamber transmission knot Structure, controlled nucleon operated belt conveyor scale follow following mathematical relationship:
N=N0 × exp (- μm0tm) (2)
N indicates that ionisation chamber counts when material in formula, and N0 indicates that ionisation chamber counts when empty belt, μm0It indicates137Cs radioactive sources Corresponding mass attentuation coefficient can then be derivedBy tmIt brings formula 1 into, then can obtain:
In formulaWhen material composition composition transfer is little, this proportionality coefficient is approximately constant, this Sample we only require to obtain constant kEi, the attenuation degree of characteristic gamma ray power spectrum is can be obtained by counting N, N0 of ionisation chamber, Then power spectrum is modified.
Mass attentuation coefficient and linear absorption coefficient relationship are as follows:
μm=μ/ρ (4)
μ in formulamFor mass attentuation coefficient, μ is linear absorption coefficient, and ρ is material density.
The linear absorption coefficient μ of substance is defined as follows:
N in formulaiIndicate the atom number density of i-th kind of element in substance,For the gammaphoton and the element of i-th kind of element Reaction cross-section, m indicate substance be made of m kind elements.
NiCalculation formula it is as follows:
M in formulaρIndicate the mass density of substance, MiIndicate Elements Atom amount, fiIndicate that i-th kind of element is shared in substance Ratio (after normalization).
We are only it is to be understood that the substantially element constituent of measured matter in this way, according to the anti-of gammaphoton and various elements The curve of section-gamma energy is answered, can be calculated by formula 4, formula 5, formula 6137The corresponding quality of Cs radioactive sources Attenuation coefficient mum0With mass attentuation coefficient μ of the characteristic gamma ray in material that energy is EimEi, and then obtain proportionality constant kEiWith the relation curve of gamma energy, N, N0 are counted according to ionisation chamber and formula 3 can be realized and be repaiied to the compensation of power spectrum Just.
Advantageous effect:
Operation is compensated to the characteristic gamma ray power spectrum of PGNAA equipment using the present invention, characteristic gamma is solved and penetrates The problem of line energy spectrum distortion, the accuracy of detection of PGNAA equipment can be promoted.
Description of the drawings:
Fig. 1 is schematic diagram of the present invention, and Fig. 2 is each element photon cross section curve graph, and Fig. 3 is proportionality constant k after calculatingECurve Figure, Fig. 4 are the front and back characteristic gamma ray energy spectrum diagram of compensation.
1-PGNAA equipment, 2-PGNAA computing hosts, 3- belt conveyors, 4- tested materials, 5-137Cs radioactive sources, 6- ionization Room.
Specific implementation:
This backoff algorithm specific implementation is made of two parts:Calculate proportionality constant kEiMatrix, compensation operation.
1, proportionality constant k is calculatedEiMatrix
Herein we assume that measured matter is cement slurry, it is assumed that characteristic gamma ray results from tested material thickness At center, cement slurry is mainly by CaCO3、SiO2、Al2O3、Fe2O3、H2O is constituted, and each substance approximate composition is shown in Table 1, is then tested Seven kinds of elements of H, C, O, Al, Si, Ca, Fe are mainly contained in material, and each element ratio f is calculated according to oxide componentsiIt is shown in Table 2, Each element photon cross section curve graph is shown in Fig. 2.
1 raw ingredients of cement content table of table
Substance CaCO3 SiO2 Al2O3 Fe2O3 H2O
Mass ratio 75% 15% 3% 2% 5%
2 cement slurry Elements Atom ratio f of tablei
Element Ratio fi
Ca 0.126127
Si 0.042042
Al 0.009892
Fe 0.004204
H 0.093427
C 0.126127
O 0.598181
According to known each element photon cross section data, each element atomic weight, each element ratio and formula 6, formula 5, Formula 4 can calculate137The corresponding mass attentuation coefficient μ of Cs radioactive sourcesm0With energy be Ei characteristic gamma ray in material Mass attentuation coefficient μmEi, and then obtain proportionality constant kEi(i=1~1024, corresponding 10keV~10.24MeV energy) matrix, kECurve is shown in Fig. 3.
μm=μ/ρ (4)
2, compensation operation
Known features gamma ray spectroscopy IEi(i=1~1024), constant kEi(i=1~1024), ionisation chamber signal N, N0, you can the characteristic gamma ray power spectrum I0 after compensation is calculated by formula 3Ei(i=1~1024).
In cement slurry detection application, the power spectrum region that we compare care is 2.8MeV~10.24MeV, therefore I This subregion power spectrum only compensated into operation when calculating, as shown in figure 4, curve I is actual measurement cement slurry power spectrum (2.8MeV~10.24MeV amplify 15 times), curve I0 be spectrum curve after compensation calculation (compensation calculation section be 2.8MeV~ 10.24MeV, this interval curve amplify 15 times).

Claims (1)

1. a kind of PGNAA characteristic gamma rays power spectrum backoff algorithm, which is characterized in that include the following steps:
Step 1: according to measured matter elemental composition ratio, each element photon reaction cross-section and mass attentuation coefficient and linearly Absorption coefficient relationship, substance linear absorption coefficient define and calculate separately energy in 2.8-10.24 with the atom number density of element Mass attentuation coefficient of the gamma-rays of MeV in the various elements of measured matterWith137The γ of 0.662 MeV of Cs radioactive sources Mass attentuation coefficient of the ray in the various elements of measured matter, according to formulaCalculate proportionality constant kEi,Wherein i=1 ~ 1024 of Ei;
Step 2: on controlled nucleon operated belt conveyor scale137Cs radioactive sources are in ionisation chamber(6)Formed belt on have tested material band information carrying N and It is the airborne signals N0 of sky on belt;
Step 3: PGNAA equipment measures the neutron activation Characteristic γ ray power spectrum I of tested material on beltEi, wherein i=1 of Ei ~1024;
Step 4: utilizing formulaCalculate the Characteristic γ ray power spectrum after compensating approachIts I=1~1024 of middle Ei.
CN201610886933.4A 2016-10-11 2016-10-11 A kind of PGNAA characteristic gamma rays power spectrum backoff algorithm Expired - Fee Related CN106290429B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610886933.4A CN106290429B (en) 2016-10-11 2016-10-11 A kind of PGNAA characteristic gamma rays power spectrum backoff algorithm

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610886933.4A CN106290429B (en) 2016-10-11 2016-10-11 A kind of PGNAA characteristic gamma rays power spectrum backoff algorithm

Publications (2)

Publication Number Publication Date
CN106290429A CN106290429A (en) 2017-01-04
CN106290429B true CN106290429B (en) 2018-10-09

Family

ID=57718586

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610886933.4A Expired - Fee Related CN106290429B (en) 2016-10-11 2016-10-11 A kind of PGNAA characteristic gamma rays power spectrum backoff algorithm

Country Status (1)

Country Link
CN (1) CN106290429B (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108645880B (en) * 2018-05-11 2021-02-02 南京航空航天大学 Energy spectrum analysis method for large-volume sample
CN112432965A (en) * 2019-08-10 2021-03-02 丹东东方测控技术股份有限公司 Method for on-line detection of sinter components
CN112392454B (en) * 2020-11-16 2023-02-03 中国石油大学(华东) Fracture bulk density quantitative calculation method based on neutron activation analysis self-shielding correction
CN115616010B (en) * 2022-12-19 2023-03-21 合肥金星智控科技股份有限公司 Material component detection method and detection device based on cross-belt neutron activation analysis

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1892252A (en) * 2005-06-27 2007-01-10 通用电气公司 Gamma and neutron radiation detector
CN204556840U (en) * 2015-04-20 2015-08-12 清华大学 Distinguish the on-line measurement device of uranium ore

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7152002B2 (en) * 2002-06-03 2006-12-19 Sabia, Inc. Method and apparatus for analysis of elements in bulk substance
US9291580B2 (en) * 2014-07-11 2016-03-22 Sabia Inc. Prompt gamma neutron activation substance analyzers

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1892252A (en) * 2005-06-27 2007-01-10 通用电气公司 Gamma and neutron radiation detector
CN204556840U (en) * 2015-04-20 2015-08-12 清华大学 Distinguish the on-line measurement device of uranium ore

Non-Patent Citations (5)

* Cited by examiner, † Cited by third party
Title
不同材料对γ射线衰减系数的MCNP模拟;刘自霞 等;《核电子学与探测技术》;20131130;第33卷(第11期);第1376-1380页 *
中子场及γ射线自吸收在PGNAA测量中的影响研究;程璨 等;《原子能科学技术》;20141031;第48卷;第802-806页 *
中子活化分析中煤样厚度及探测器位置的选择;王二永 等;《吉林大学学报》;20150930;第53卷(第5期);第1031-1033页 *
大样品中子活化分析中γ衰减系数的研究;张海青 等;《第十二届全国活化分析学术交流会》;20101018;第35页第1-7段 *
大样品中子活化分析的理论依据和误差修正;张海青 等;《原子能科学技术》;20101031;第44卷(第10期);第1238-1242页 *

Also Published As

Publication number Publication date
CN106290429A (en) 2017-01-04

Similar Documents

Publication Publication Date Title
CN106290429B (en) A kind of PGNAA characteristic gamma rays power spectrum backoff algorithm
CN104198503B (en) Online coal ash content measurement system and method based on natural gamma rays
Quarati et al. Study of 138La radioactive decays using LaBr3 scintillators
Maienschein et al. Gamma rays associated with fission
Akkurt et al. Chemical corrosion on gamma-ray attenuation properties of barite concrete
JPS5853732B2 (en) Coal analysis method
CN101349660A (en) On-line analysis detection method of mine material iron ore grade
Morishita et al. Development of a Si-PM based alpha camera for plutonium detection in nuclear fuel facilities
VanDevender et al. High-Purity Germanium Spectroscopy at Rates in Excess of $10^{6} $ Events/s
Amatullah et al. Assessment of radiometric standard and potential health risks from building materials used in Bangladeshi dwellings
GB1560970A (en) On-line system for monitoring sheet material additives
Mosset et al. Evaluation of two thermal neutron detection units consisting of ZnS/6LiF scintillating layers with embedded WLS fibers read out with a SiPM
US9518941B1 (en) Weight-percent analysis for prompt gamma neutron activation substance analyzers
JPS5832150A (en) Measuring device for measuring concentration of one element in sample and its method
CN104504273A (en) Energy spectrum processing method capable of increasing gamma-ray peak detection sensitivity
CN112444533B (en) Method for detecting moisture content and element content in sintered material
CN112444532B (en) Method for measuring total iron content in sintered material on line
Moreira et al. Determination of 51Cr and 241Am X-ray and gamma-ray emission probabilities per decay
Avdeichikov et al. Systematics in the light response of BGO, CsI (Tl) and GSO (Ce) scintillators to charged particles
Szücs et al. Comparison of two HPGe counting system used in activation studies for nuclear astrophysics
Kim et al. Measurement of low-energy events due to 222Rn daughter contamination on the surface of a NaI (Tl) crystal
CN111158040A (en) Layout structure for improving compton inhibition factor of anti-well-being spectrometer
JPS6171341A (en) Component analyzing method
Vo Comparison of portable detectors for uranium enrichment measurements
CN112432965A (en) Method for on-line detection of sinter components

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
CB03 Change of inventor or designer information
CB03 Change of inventor or designer information

Inventor after: Lu Jingbin

Inventor after: Zhao Long

Inventor after: Xu Xu

Inventor before: Zhao Long

Inventor before: Lu Jingbin

Inventor before: Xu Xu

CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20181009

Termination date: 20201011