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现行 ASTM C1030-10(2018)
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Standard Test Method for Determination of Plutonium Isotopic Composition by Gamma-Ray Spectrometry 通过γ射线光谱法测定钚同位素组成的标准测试方法
发布日期: 2018-04-01
1.1 本试验方法适用于测定同位素均匀含钚材料中的同位素丰度。本试验方法可适用于其他含钚材料,其中一些材料可能需要修改所述试验方法。 1.2 该程序适用于包含钚质量从几十毫克到临界极限允许的最大钚质量的物品。 1.3 钚的可测量γ射线发射涵盖了约30千电子伏到800千电子伏以上的能量范围。 钚及其子体的K-X射线发射在100keV左右的区域。该试验方法已应用于这一广谱排放的所有部分。 1.4 同位素丰度 242 钚同位素没有有用的伽马射线特征,因此不能直接测定。同位素相关技术可用于估算其相对丰度参考值 ( 1. ) 和 ( 2. ) . 2. 1.5 该测试方法已在常规使用中证明,同位素丰度范围为99至<50 % 239 聚氨基甲酸酯。该测试方法也适用于该范围以外的同位素丰度。 1.6 以国际单位制表示的数值应视为标准值。本标准不包括其他计量单位。 1.7 本标准并非旨在解决与其使用相关的所有安全问题(如有)。本标准的用户有责任在使用前制定适当的安全、健康和环境实践,并确定监管限制的适用性。 1.8 本国际标准是根据世界贸易组织技术性贸易壁垒(TBT)委员会发布的《关于制定国际标准、指南和建议的原则的决定》中确立的国际公认标准化原则制定的。 ====意义和用途====== 4.1 通过γ射线光谱法测定钚同位素组成是一种非破坏性技术,当与其他非破坏性技术,如量热法(试验方法)一起使用时 C1458 )或中子计数(试验方法 C1207 , C1316 , C1493 和 C1500 ),可以提供材料核算和保障需要所需的全无损钚分析。 4.2 由于伽马射线光谱测定系统通常是自动化的,因此测试方法的常规使用快速、可靠,并且不需要劳动密集型。该测试方法是非破坏性的,不需要样品制备,并且不会产生废物处理问题。 4.3 本试验方法假设被测项目中的所有钚具有相同的同位素分布,通常称为同位素同质性(见 7.2.4 和 7.2.5 ). 4.4 这个 242 钚丰度不是通过该测试方法测量的,必须通过同位素相关技术、流平均值、历史信息或其他测量技术进行估计。 4.5 镅-241是 241 聚氨基甲酸酯。这个 241 Am公司/ 239 钚原子比也可以通过该试验方法确定(假设钚和钚的同位素分布均匀) 241 Am)。确定 241 Am公司/ 239 钚原子比是正确解释量热测量的必要条件。 4.6 给定批次或项目钚的同位素成分是该项目的一个属性,一旦确定,可用于后续库存测量,以验证测量不确定性范围内项目的身份。 4.7 该方法还可以测量其他γ发射同位素与钚的比率,假设它们与项目中的钚具有相同的空间分布。其中一些“其他”γ辐射同位素包括铀、镎、curium、铯和其他裂变产物的同位素。 本标准的相同方法可用于测量仅含铀项目中铀的同位素组成 ( 3. , 4. , 5. , 6. ) .
1.1 This test method is applicable to the determination of isotopic abundances in isotopically homogeneous plutonium-bearing materials. This test method may be applicable to other plutonium-bearing materials, some of which may require modifications to the described test method. 1.2 The procedure is applicable to items containing plutonium masses ranging from a few tens of milligrams up to the maximum plutonium mass allowed by criticality limits. 1.3 Measurable gamma ray emissions from plutonium cover the energy range from approximately 30 keV to above 800 keV. K-X-ray emissions from plutonium and its daughters are found in the region around 100 keV. This test method has been applied to all portions of this broad spectrum of emissions. 1.4 The isotopic abundance of the 242 Pu isotope is not directly determined because it has no useful gamma-ray signature. Isotopic correlation techniques may be used to estimate its relative abundance Refs ( 1 ) and ( 2 ) . 2 1.5 This test method has been demonstrated in routine use for isotopic abundances ranging from 99 to <50 % 239 Pu. This test method has also been employed for isotopic abundances outside this range. 1.6 The values stated in SI units are to be regarded as standard. No other units of measurement are included in this standard. 1.7 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety, health, and environmental practices and determine the applicability of regulatory limitations prior to use. 1.8 This international standard was developed in accordance with internationally recognized principles on standardization established in the Decision on Principles for the Development of International Standards, Guides and Recommendations issued by the World Trade Organization Technical Barriers to Trade (TBT) Committee. ====== Significance And Use ====== 4.1 The determination of plutonium isotopic composition by gamma-ray spectrometry is a nondestructive technique and when used with other nondestructive techniques, such as calorimetry (Test Method C1458 ) or neutron counting (Test Methods C1207 , C1316 , C1493 , and C1500 ), can provide a wholly nondestructive plutonium assay necessary for material accountancy and safeguards needs. 4.2 Because gamma-ray spectrometry systems are typically automated, the routine use of the test method is fast, reliable, and is not labor intensive. The test method is nondestructive, requires no sample preparation, and does not create waste disposal problems. 4.3 This test method assumes that all plutonium in the measured item has the same isotopic distribution, often called isotopic homogeneity (see 7.2.4 and 7.2.5 ). 4.4 The 242 Pu abundance is not measured by this test method and must be estimated from isotopic correlation techniques, stream averages, historical information, or other measurement techniques. 4.5 Americium-241 is a daughter product of 241 Pu. The 241 Am/ 239 Pu atom ratio can also be determined by means of this test method (assuming a homogeneous isotopic distribution of plutonium and 241 Am). The determination of the 241 Am/ 239 Pu atom ratio is necessary for the correct interpretation of a calorimetric heat measurement. 4.6 The isotopic composition of a given batch or item of plutonium is an attribute of that item and, once determined, can be used in subsequent inventory measurements to verify the identity of an item within the measurement uncertainties. 4.7 The method can also measure the ratio of other gamma-emitting isotopes to plutonium assuming they have the same spatial distribution as the plutonium in the item. Some of these “other” gamma-emitting isotopes include isotopes of uranium, neptunium, curium, cesium, and other fission products. The same methods of this standard can be used to measure the isotopic composition of uranium in items containing only uranium ( 3 , 4 , 5 , 6 ) .
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归口单位: C26.10
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