ASTM D5411-10(2015)由美国材料与试验协会 US-ASTM 发布于 2010。
5.1 This practice is useful for the determination of the average energy per disintegration of the isotopic mixture found in the reactor-coolant system of a nuclear reactor (1).4 The E value is used to calculate a site-specific activity limit for the reactor coolant system, generally identified as
where K = a power reactor site specific constant (usually in the range of 50 to 200). The activity of the reactor coolant system is routinely measured, then compared to the value of Alimiting. If the reactor coolant activity value is less than Alimiting then the 2-h radiation dose, measured at the plant boundary, will not exceed an appropriately small fraction of the Code of Federal Regulations, Title 10, part 100 dose guidelines. It is important to note that the measurement of the reactor coolant system radioactivity is determined at a set frequency by use of gamma spectrometry only. Thus the radionuclides that go into the calculation of E and subsequently Alimiting are only those that are calculated using gamma spectrometry.5.2 In calculating E, the energy dissipated by beta particles (negatrons and positrons) and photons from nuclear decay of beta-gamma emitters. This accounting includes the energy released in the form of energy released from extra-nuclear transitions in the form of X-rays, Auger electrons, and conversion electrons. However, not all radionuclides present in a sample are included in the calculation of E.
5.3 Individual, nuclear reactor, technical specifications vary and each nuclear operator must be aware of limitations affecting their plant operation. Typically, radioiodines, radionuclides with half lives of less than 10 min (except those in equilibrium with the parent), and those radionuclides, identified using gamma spectrometry, with less than a 958201;% confidence level, are not typically included in the calculation. However, the technical requirements are that the reported activity must account for at least 958201;% of the activity after excluding radioiodines and short-lived radionuclides. There are individual bases for each exclusion.
5.3.1 Radioiodines are typically excluded from the calculation of E because United States commercial nuclear reactors are required to operate under a more conservative restriction of 1 μC (37 kBq) per gram dose equivalent 131I (DEI) in the reactor coolant.
只要包壳不破损,芯块不熔化,这些放射性物质就不会逸出到环境中。 其次是衰变热。反应堆停闭后,堆芯内中子链式裂变反应虽然中止,但是,裂变产物继续衰变,这些裂变产物的半衰期有的很长,射线在与周围物质作用时由于受到阻挡而释放出热量,这就是衰变热。由于反应堆在停堆后,还有一定量的功率,因此反应堆必须设置停堆余热排出系统来保证反应堆的安全。...
下面为与放药相关的一些主要衰变类型:α衰变:原子核放射α粒子(He核)的放射性衰变。β-衰变:原子核发射电子(e)的放射性衰变。β+衰变:原子核发射正电子(e+)的放射性衰变。EC衰变:电子俘获衰变。原子核俘获轨道电子并放射中微子的放射性衰变。 IT衰变:同质异能跃迁衰变。一种同质异能素变为另一个能量较低的同质异能素的放射性衰变。放射性衰变服从一定规律,单一的放射性衰变遵从指数衰变规律。...
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