CN103257147A - 232Method for measuring U - Google Patents

232Method for measuring U Download PDF

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CN103257147A
CN103257147A CN2012100358328A CN201210035832A CN103257147A CN 103257147 A CN103257147 A CN 103257147A CN 2012100358328 A CN2012100358328 A CN 2012100358328A CN 201210035832 A CN201210035832 A CN 201210035832A CN 103257147 A CN103257147 A CN 103257147A
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alpha
uranium
sample
source
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CN103257147B (en
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王琛
赵永刚
李力力
朱留超
赵兴红
常志远
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China Institute of Atomic of Energy
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China Institute of Atomic of Energy
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Abstract

The invention belongs to the technical field of analytical chemistry and discloses a method for preparing a high-purity gold-silver-copper alloy232Method for measuring U. The method comprises the following steps: (1) dissolving a uranium sample by using nitric acid, and electroplating to prepare an alpha source of the uranium sample; (2) measuring alpha energy spectrum of alpha source of uranium sample by using alpha spectrometer to obtain234U、235U、236U and238total count of U NZAnd deduction228After Th contribution232Alpha count of U; (3) putting the dissolved uranium sample into a mass spectrometer for analysis234U、235U、236U and238u accounts for the atomic percent of uranium; (4) calculating the content of uranium in the uranium sample according to the formula (7)232The content of U. The method is simple to operate and accurate in determination.

Description

232The assay method of U
Technical field
The invention belongs to technical field of analytical chemistry, be specifically related to 232The assay method of U.
Background technology
The isotope of uranium is generally in the uranium sample after the reactor irradiation 232U, 233U, 234U, 235U, 236U, 238U.Group's part uranium isotope wherein 232U, 233U, 234U, 236The existence of U and daughter thereof brings irradiation and pollution problem for nuclear fuel cycle and nuclear fuel element manufacturing, has increased the protection difficulty, especially 232U, its half life period, energy of height, thermal neutron absorption cross section short, that decay daughter produces were big, were the uranium isotopes of strict restriction during element is made.In the uranium sample after the reactor irradiation of U.S. ASTM standard regulation 232The maximum limit value of U is 0.005 μ g/gU.In order accurately to measure in the uranium sample 232U, it is the standard test method of ASTM C761-96 that U.S.'s test can have been set up label with materialogy, China also adopting by equivalent ASTM C761-88 has set up nuclear industry standard EJ 727-1992, these two kinds of standards all are to adopt the quality of uranium in the colorimetric method for determining electro-deposition source, use the alpha energy spectrum method to measure the electro-deposition source 232The U quality.But the method is comparatively loaded down with trivial details, when determining the quality of uranium in the electro-deposition source, and the curve of need working, and must carry out colorimetric estimation when determining each sedimentary origin quality.
Summary of the invention
The present invention is directed to the problem that above technology exists, proposed a kind of 232The assay method of U, this method is simple to operate, measurement is accurate.
The present invention adopts alpha energy spectrum and mass spectrometry to measure after the reactor irradiation in the uranium sample 232The content of U.
Measure and to record by alpha energy spectrum 234U, 235U, 236U, 238Total α counting of U.Because 232U discharges two kinds of α particles, and energy is respectively 5.28MeV and 5.32MeV, with 228The energy of Th is the alpha ray overlaid of 5.34MeV, but can pass through 228Another energy of Th is the alpha ray deduction of 5.42MeV 228Th is right 232The contribution of U obtains 232The counting of U. 232After the quality of U can be used and deduct 232The α counting of U calculates with its intrinsic specific activity, and its computing formula is as follows:
m 232=A 232232=(N 5.3-0.3767·N 5.42)/(t·α 232·Ef) (1)
In the formula (1):
m 232, A 232, α 232Be respectively in the sample 232The quality of U, 232U activity, 232The intrinsic specific activity of U;
T, Ef are respectively Measuring Time and the detector efficiency of alpha energy spectrum instrument;
N 5.3For 232The 5.26MeV of U, 5.32MeV reach 228Total α counting at the 5.34MeV α peak of Th;
N 5.42For 228The clean counting at the 5.42MeV α peak of Th.
Measure in the uranium sample by many receiving inductances coupled plasma mass spectrometer 232U, 233U, 234U, 235U, 236U and 238U accounts for the U elements atomic percentage, because 232U, 233The shared atomic percent of U is too little, can ignore.With 234U is example, and its specific activity and Mass Calculation formula are as follows:
A 234=m 234·α 234 (2)
A 234=N 234·/(t·Ef) (3)
m 234 = m U · n 234 % · M 234 / Σ i M i · n i % , ( i = 234,235,236,238 ) - - - ( 4 )
In the formula (4):
N 234For 234The α counting of U;
n 234%For 234U account for the U element atomic percent;
M 234For 234The atomic weight of U;
m UQuality for U in the sample.
With (3), (4) two formulas are brought (2) formula into, get formula (5):
N 234 = m u · n 234 % · M 234 · α 234 · t · Ef Σ i M i · n i % , ( i = 234,235,236,238 ) - - - ( 5 )
In alpha energy spectrum figure, can obtain 234U, 235U, 236U and 238The tale N of U z=N 234+ N 235+ N 236+ N 238So, can be right 235U, 236U and 238U derives the formula same with formula (5), and the two ends addition of several formula can be derived:
m u = N z · Σ i M i · n i % t · Ef · Σ i M i · n i % · α i , ( i = 234,235,236,238 ) - - - ( 6 )
Can draw computing formula (7) by (1) formula and (6) formula:
m 232 m U = ( N 5.3 - 0.3767 · N 5.42 ) · Σ i M i · n i % · α i α 232 · N z · Σ i M i · n i % , ( i = 234,235,236,238 ) - - - ( 7 )
Only can find out from formula (7) needs sample is carried out alpha energy spectrum and mass-spectrometer measurement can calculate the sample 232The content of U.
The present invention is achieved by the following technical solutions:
(1) with the uranium sample nitric acid dissolve, and electroplates the uranium sample α source of making;
(2) use alpha spectrometer to measure the alpha energy spectrum in uranium sample α source, obtain 234U, 235U, 236U and 238Total α counting N of U ZAnd deduction 228After the Th contribution 232The α counting of U;
(3) uranium sample after will dissolving is put into mass spectrometer analysis 234U, 235U, 236U and 238U account for element U atomic percent;
(4) according to formula
m 232 m U = ( N 5.3 - 0.3767 · N 5.42 ) · Σ i M i · n i % · α i α 232 · N z · Σ i M i · n i % , ( i = 234,235,236,238 )
Calculate in the uranium sample 232The content of U.
Adopt in the measurement uranium sample provided by the invention 232The method of U, the beneficial effect that has is: (1) is simple to operate.This method only needs carrying out power spectrum and mass spectrophotometry behind the sample source processed, need not to carry out complicated colorimetric estimation, and need not the curve of working; (2) measure accurately.Because this method has been introduced mass spectrometer sample has been analyzed, and has improved accuracy, has reduced the uncertainty of analysis result.
Description of drawings
The alpha energy spectrum figure of accompanying drawing 1 uranium sample.
Embodiment
Below in conjunction with embodiment and Figure of description the technical program is further elaborated.
Embodiment 1
At first with the uranium sample dissolving, adding 5ml concentration in galvanic deposition cell is the (NH of 0.025mol/L 4) 2C 2O 4With 5ml concentration be the HNO of 0.15mol/L 3As electrodeposit liquid, add 30 microgram uranium simultaneously, and to regulate electrodeposit liquid pH value with ammoniacal liquor be 1.0, electro-deposition is 4 hours in ice-water bath, and it is 30 μ g/cm that surface density is made in plating 2The α source.
Use the semiconductor alpha spectrometer to measure then 234U, 235U, 236U, 238Total α counting N of U ZAnd deduction 228After the Th contribution 232The α counting of U, Measuring Time is 24 hours.
The dilution of uranium sample after will dissolving at last, and with many receiving inductances coupled plasma mass spectroscopy uranium isotope atomic percent.Optimize instrument with natural uranium solution, select for use the standard that approaches with the sample abundance to proofread and correct actual sample, finally obtain in the sample 234U, 235U, 236U and 238U accounts for the atomic percent of element U, calculates and can calculate in the uranium sample according to following formula 232The content of U.
m 232 m U = ( N 5.3 - 0.3767 · N 5.42 ) · Σ i M i · n i % · α i α 232 · N z · Σ i M i · n i % , ( i = 234,235,236,238 )
Measure 232The content of U is 1.118 * 10 -9g 232The known sample of U/gU, final measurement are (1.118 * 10 -9± 9.0 * 10 -11) g 232U/gU (k=2), and mass spectrum is contributed less than 1% its overall uncertainty.The result shows, adopts mass spectrum in the uranium sample 232It is higher that U analyzes the accuracy that obtains.
Embodiment 2
Identical with embodiment 1 method therefor, step, different is the pH value of electrodeposit liquid, measures 232The content of U is 1.118 * 10 -9g 232The known sample of U/gU, the result of gained is:
Under the different condition of table 1 electrodeposit liquid pH value 232The assay value (k=2) of U
The pH value of electrodeposit liquid 232U content (g/g)
1.5 1.118×10 -9±9.2×10 -11
2.0 1.118×10 -9±10×10 -11
Embodiment 2
Identical with embodiment 1 method therefor, step, different is the time in plating source processed, and the result of gained is:
Under the different condition of table 2 electroplating time 232The assay value (k=2) of U
Electroplating time (hour) 232U content (g/g)
3 1.118×10 -9±8.8×10 -11
5 1.118×10 -9±9.4×10 -11
Embodiment 2
Identical with embodiment 1 method therefor, step, different is the Measuring Time of alpha spectrometer, and the result of gained is:
Under the different condition of table 3 alpha spectrometer Measuring Time 232The assay value (k=2) of U
The alpha spectrometer Measuring Time (hour) 232U content (g/g)
22 1.118×10 -9±9.3×10 -11
26 1.118×10 -9±9.4×10 -11
Adopt the result of technical scheme gained provided by the invention accurate, measure simply.

Claims (6)

1. 232The assay method of U is characterized in that, this method may further comprise the steps:
(1) uranium sample is made the α source;
(2) use alpha spectrometer to measure the alpha energy spectrum in uranium sample α source, obtain 234U, 235U, 236U and 238The tale N of U ZAnd 232The α counting of U;
(3) will put into mass spectrometer analysis after the uranium sample dissolving 234U, 235U, 236U and 238U accounts for the atomic percent of uranium element;
(4) according to formula
m 232 m U = ( N 5.3 - 0.3767 · N 5.42 ) · Σ i M i · n i % · α i α 232 · N z · Σ i M i · n i % , ( i = 234,235,236,238 )
Calculate in the uranium sample 232The content of U.
2. according to claim 1 232The assay method of U is characterized in that, the uranium sample in the described step (1) is earlier with being prepared into the α source behind the nitric acid dissolve again.
3. according to claim 1 232The assay method of U is characterized in that, the method that prepare the α source in the described step (1) is for electroplating, and the pH value of used electrodeposit liquid is 1.0~2.0 during plating.
4. the assay method of 232U according to claim 1 is characterized in that, the electroplating time in plating source processed is 3~5 hours in the described step (1).
5. according to claim 1 232The assay method of U is characterized in that, the Measuring Time of alpha spectrometer is 22~26 hours in the described step (2).
6. according to claim 1 232The assay method of U is characterized in that, mass spectrometer used in the described step (3) for accepting icp ms more.
CN201210035832.8A 2012-02-17 2012-02-17 232Method for measuring U Active CN103257147B (en)

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Cited By (7)

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Publication number Priority date Publication date Assignee Title
CN103528868A (en) * 2013-10-22 2014-01-22 核工业二四〇研究所 Uranium isotope ratio analysis and source production method
CN104035118A (en) * 2014-06-25 2014-09-10 中国原子能科学研究院 Uranium content detection method
CN104316510A (en) * 2014-10-29 2015-01-28 中国原子能科学研究院 Raman spectrum analysis method of sexivalent uranium
CN105738386A (en) * 2016-03-09 2016-07-06 陈立 Method for analyzing total quantity of light-rear-earth lanthanum metal and its compounds by using Gamma-spectroscopy
CN105806854A (en) * 2016-03-09 2016-07-27 邓晓钦 Method for analyzing grades of light rare earth ore and concentrate thereof by gamma energy spectrum method
CN107389661A (en) * 2017-07-24 2017-11-24 中国科学院上海应用物理研究所 A kind of method of uranium isotope composition on quick measure α disks
CN110261210A (en) * 2019-07-31 2019-09-20 核工业二三O研究所 The alpha energy spectrum method of testing of the method for separating and concentrating of uranium and uranium in sample of sandstone

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Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103528868A (en) * 2013-10-22 2014-01-22 核工业二四〇研究所 Uranium isotope ratio analysis and source production method
CN103528868B (en) * 2013-10-22 2016-01-27 核工业二四〇研究所 A kind of uranium isotope ratio analysis source side method
CN104035118A (en) * 2014-06-25 2014-09-10 中国原子能科学研究院 Uranium content detection method
CN104316510A (en) * 2014-10-29 2015-01-28 中国原子能科学研究院 Raman spectrum analysis method of sexivalent uranium
CN105738386A (en) * 2016-03-09 2016-07-06 陈立 Method for analyzing total quantity of light-rear-earth lanthanum metal and its compounds by using Gamma-spectroscopy
CN105806854A (en) * 2016-03-09 2016-07-27 邓晓钦 Method for analyzing grades of light rare earth ore and concentrate thereof by gamma energy spectrum method
CN107389661A (en) * 2017-07-24 2017-11-24 中国科学院上海应用物理研究所 A kind of method of uranium isotope composition on quick measure α disks
CN110261210A (en) * 2019-07-31 2019-09-20 核工业二三O研究所 The alpha energy spectrum method of testing of the method for separating and concentrating of uranium and uranium in sample of sandstone

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