ASTM D2460-2007 Standard Test Method for Alpha-Particle-Emitting Isotopes of Radium in Water《水中镭的阿尔法粒子幅射同位素用标准试验方法》.pdf
《ASTM D2460-2007 Standard Test Method for Alpha-Particle-Emitting Isotopes of Radium in Water《水中镭的阿尔法粒子幅射同位素用标准试验方法》.pdf》由会员分享,可在线阅读,更多相关《ASTM D2460-2007 Standard Test Method for Alpha-Particle-Emitting Isotopes of Radium in Water《水中镭的阿尔法粒子幅射同位素用标准试验方法》.pdf(7页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: D 2460 07Standard Test Method forAlpha-Particle-Emitting Isotopes of Radium in Water1This standard is issued under the fixed designation D 2460; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the year of last revision
2、. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon (e) indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method covers the separation of dissolvedradium from water for the purpose of measuring its radioac-tivity. Although all
3、 radium isotopes are separated, the testmethod is limited to alpha-particle-emitting isotopes by choiceof radiation detector. The most important of these radioisotopesare223Ra,224Ra, and226Ra. The lower limit of concentration towhich this test method is applicable is 3.7 3 10-2Bq/L(1 pCi/L).1.2 This
4、 test method may be used for absolute measure-ments by calibrating with a suitable alpha-emitting radioiso-tope such as226Ra, or for relative methods by comparingmeasurements with each other. Mixtures of radium isotopesmay be reported as equivalent226Ra. Information is alsoprovided from which the re
5、lative contributions of radiumisotopes may be calculated.1.3 This standard does not purport to address all of thesafety concerns, if any, associated with its use. It is theresponsibility of the user of this standard to establish appro-priate safety and health practices and determine the applica-bili
6、ty of regulatory limitations prior to use. For a specificprecautionary statement, see Section 9.2. Referenced Documents2.1 ASTM Standards:2C 859 Terminology Relating to Nuclear Materials3D 1129 Terminology Relating to WaterD 1193 Specification for Reagent WaterD 1943 Test Method for Alpha Particle R
7、adioactivity ofWaterD 2777 Practice for Determination of Precision and Bias ofApplicable Test Methods of Committee D19 on WaterD 3370 Practices for Sampling Water from Closed ConduitsD 3454 Test Method for Radium-226 in WaterD 3648 Practices for the Measurement of RadioactivityD 4448 Guide for Sampl
8、ing Ground-Water MonitoringWellsD 5847 Practice for Writing Quality Control Specificationsfor Standard Test Methods for Water AnalysisD 6001 Guide for Direct-Push Ground Water Sampling forEnvironmental Site Characterization3. Terminology3.1 Definition:3.1.1 For definitions of terms used in this stan
9、dard, seeTerminologies C 859 and D 1129. For terms not included inthese, reference may be made to other published glossaries (1,2).44. Summary of Test Method4.1 Radium is collected from the water by coprecipitationwith mixed barium and lead sulfates. The barium and leadcarriers are added to a soluti
10、on containing alkaline citrate ionwhich prevents precipitation until interchange has taken place.Sulfuric acid is then used to precipitate the sulfates, which arepurified by nitric acid washes. The precipitate is dissolved inammoniacal EDTA. The barium and radium sulfates arereprecipitated by the ad
11、dition of acetic acid, thereby separatingthem from lead and other radionuclides. The precipitate isdried on a planchet, weighed to determine the chemical yield,and alpha-counted to determine the total disintegration rate ofalpha-particle-emitting radium isotopes. This procedure isbased upon publishe
12、d ones (3, 4).5. Significance and Use5.1 Radium is one of the most radiotoxic elements. Itsisotope of mass 226 is the most hazardous because of its longhalf-life. The isotopes 223 and 224, although not as hazardous,are of some concern in appraising the quality of water.5.2 The alpha-particle-emittin
13、g isotopes of radium otherthan that of mass 226 may be determined by difference ifradium-226 is measured separately, such as by Test MethodD 3454. Note that one finds226Ra and223Ra together invariable proportions (5, 6), but224Ra does not normally occurwith them. Thus,223Ra often may be determined b
14、y simply1This test method is under the jurisdiction of ASTM Committee D19 on Waterand is the direct responsibility of Subcommittee D19.04 on Methods of Radiochemi-cal Analysis.Current edition approved June 15, 2007. Published July 2007. Originallyapproved in 1966. Replaces D 246066 T. Last previous
15、edition approved in 2005as D 2460 05.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.3Withdrawn.4The boldface
16、 numbers in parentheses refer to the list of references at the end ofthis standard.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.subtracting the226Ra content from the total: and if226Raand223Ra are low,224Ra may be determined direc
17、tly. Thedetermination of a single isotope in a mixture is less precisethan if it occurred alone.6. Interferences6.1 A barium content in the sample exceeding 0.2 mg willbias chemical yield high and lead to falsely low sample results.6.2 The presence of suspended solids or insoluble precipi-tates whic
18、h fail to dissolve during step 12.5 will bias chemicalyield high and lead to falsely low sample results.6.3 The total alpha particle emission rate from the preparedsample changes over time. This will influence the radiumdetection efficiency of the counting system used. Initially, thetotal emission r
19、ate will increase as the short-lived radonprogeny ingrow in the processed sample. After reaching amaximum, the alpha emission rate will decline at the half lifeof the radium isotope of interest. In samples of pure isotope,maximum emission rate after radium separation is reachedafter a period of 4 ho
20、urs for223Ra, 24 hours for224Ra, and 28days for226Ra. (See Fig. 1.)6.4 The alpha particle detection efficiency decreases withincreasing precipitate mass. Controlling the precipitate massrelative to that used for calibration of the test will minimize theintroduction of significant bias into sample re
21、sults.6.5 The changing alpha emission rate and self-absorptioneffects noted in 6.3 and 6.4 can be addressed by reproducingthese conditions during the calibration of the instrument. Aseries of standards analyzed per 11.2 may be used to generatea curve describing efficiencies over a range of precipita
22、temasses and a series of time encompassing the ingrowth curve(30 days) of222Rn daughters. (See Fig. 2).7. Apparatus7.1 For suitable gas-flow proportional or alpha-scintillationcounting equipment, refer to Test Method D 1943.8. Reagents8.1 Purity of ReagentsReagent grade chemicals shall beused in all
23、 tests. Unless otherwise indicated, it is intended thatall reagents shall conform to the specifications of the Commit-tee on Analytical Reagents of the American Chemical Society,where such specifications are available.5Other grades may beused, provided it is first ascertained that the reagent is ofs
24、ufficiently high purity to permit its use without lessening theprecision, or increasing the bias, of the determination.8.2 Purity of WaterUnless otherwise indicated, referencesto water shall be understood to mean reagent water conformingto Specification D 1193, Type III.8.3 Radioactivity Purity of R
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