{"id":24475,"date":"2024-10-17T00:11:54","date_gmt":"2024-10-17T00:11:54","guid":{"rendered":"https:\/\/pdfstandards.shop\/product\/uncategorized\/astm-e705-2008-2\/"},"modified":"2024-10-24T13:32:28","modified_gmt":"2024-10-24T13:32:28","slug":"astm-e705-2008-2","status":"publish","type":"product","link":"https:\/\/pdfstandards.shop\/product\/publishers\/astm\/astm-e705-2008-2\/","title":{"rendered":"ASTM-E705 2008"},"content":{"rendered":"
Refer to Practice E 261 for a general discussion of the determination of fast-neutron fluence rate with fission detectors.<\/p>\n
237 <\/sup> Np is available as metal foil, wire, or oxide powder. For further information, see Guide E 844. It is usually encapsulated in a suitable container to prevent loss of, and contamination by, the 237 <\/sup> Np and its fission products.<\/p>\n One or more fission products can be assayed. Pertinent data for relevant fission products are given in Table 1 and Table 2.<\/p>\n 137 <\/sup> Cs- 137m <\/sup> Ba is chosen frequently for long irradiations. Radioactive products 134 <\/sup> Cs and 136 <\/sup> Cs may be present, which can interfere with the counting of the 0.662 MeV 137 <\/sup> Cs- 137m <\/sup> Ba gamma ray (see Test Methods E 320).<\/p>\n 140 <\/sup> Ba- 140 <\/sup> La is chosen frequently for short irradiations (see Test Method E 393).<\/p>\n 95 <\/sup> Zr can be counted directly, following chemical separation, or with its daughter 95 <\/sup> Nb, using a high-resolution gamma detector system.<\/p>\n 144 <\/sup> Ce is a high-yield fission product applicable to 2- to 3-year irradiations.<\/p>\n It is necessary to surround the 237 <\/sup> Np monitor with a thermal neutron absorber to minimize fission product production from trace quantities of fissionable nuclides in the 237 <\/sup> Np target and from 238 <\/sup> Np and 238 <\/sup> Pu from (n, \u03b3 <\/span> ) reactions in the 237 <\/sup> Np material. Assay of 238 <\/sup> Pu and 239 <\/sup> Pu concentration is recommended when a significant contribution is expected.<\/p>\n Fission product production in a light-water reactor by neutron activation products 238 <\/sup> Np and 238 <\/sup> Pu has been calculated to be insignificant (1.2 %), compared to that from 237 <\/sup> Np(n,f), for an irradiation period of 12 years at a fast neutron ( E <\/span> > 1 MeV) fluence rate of 1 \u00d7 <\/span> 10 11 <\/sup> cm \u2212 <\/span> 2 <\/sup> \u00b7 <\/span> s \u2212 <\/span> 1 <\/sup> , provided the 237 <\/sup> Np is shielded from thermal neutrons (see Fig. 2 of Guide E 844).<\/p>\n Fission product production from photonuclear reactions, that is, ( \u03b3 <\/span> ,f) reactions, while negligible near-power and researchreactor cores, can be large for deep-water penetrations (1). <\/span><\/p>\n Good agreement between neutron fluence measured by 237 <\/sup> Np fission and the 54 <\/sup> Fe(n,p) 54 <\/sup> Mn reaction has been demonstrated (2). <\/span> The reaction 237 <\/sup> Np(n,f) F.P. is useful since it is responsive to a broader range of neutron energies than most threshold detectors.<\/p>\n The 237 <\/sup> Np fission neutron spectrum-averaged cross section in several benchmark neutron fields are given in Table 3 of Practice E 261. Sources for the latest recommended cross sections are given in Guide E 1018. In the case of the 237 <\/sup> Np(n,f)F.P. reaction, the recommended cross section source is the ENDF\/B-VI cross section (MAT = 9346) revision 1 (3) <\/span> . Fig. 1 shows a plot of the recommended cross section versus neutron energy for the fast-neutron reaction 237 <\/sup> Np(n,f)F.P.<\/p>\n Note <\/span> 1\u2014The data are taken from the Evaluated Nuclear Data file, ENDF\/B-VI, rather than the later ENDF\/B-VII. This is in accordance with Guide E 1018 Guide for Application of ASTM Evaluated Cross Section Data File, 6.1. since the later ENDF\/B-VII data files do not include covariance information. For more details see Section H of (10) <\/span><\/p>\n A <\/span> <\/sup> The lightface numbers in parentheses are the magnitude of plus or minus uncertainties in the last digit(s) listed.<\/p>\n B <\/span> <\/sup> With 137m <\/sup> Ba (2.552 min) in equilibrium.<\/p>\n C <\/span> <\/sup> Probability of daughter 140 <\/sup> La decay.<\/p>\n D <\/span> <\/sup> With 140 <\/sup> La (1.6781 d) in transient equilibrium.<\/p>\n