ASTM E693-2012 0000 Standard Practice for Characterizing Neutron Exposures in Iron and Low Alloy Steels in Terms of Displacements Per Atom (DPA) E&thinsp 706(ID) 《根据每个原子(DPA)、E706(.pdf
《ASTM E693-2012 0000 Standard Practice for Characterizing Neutron Exposures in Iron and Low Alloy Steels in Terms of Displacements Per Atom (DPA) E&thinsp 706(ID) 《根据每个原子(DPA)、E706(.pdf》由会员分享,可在线阅读,更多相关《ASTM E693-2012 0000 Standard Practice for Characterizing Neutron Exposures in Iron and Low Alloy Steels in Terms of Displacements Per Atom (DPA) E&thinsp 706(ID) 《根据每个原子(DPA)、E706(.pdf(8页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E693 12Standard Practice forCharacterizing Neutron Exposures in Iron and Low AlloySteels in Terms of Displacements Per Atom (DPA),E 706(ID)1This standard is issued under the fixed designation E693; the number immediately following the designation indicates the year oforiginal adoption o
2、r, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1. Scope1.1 This practice describes a standard procedure for charac-terizing neutron irrad
3、iations of iron (and low alloy steels) interms of the exposure index displacements per atom (dpa) foriron.1.2 Although the methods of this practice apply to anymaterial for which a displacement cross section sd(E) is known(see Practice E521), this practice is written specifically for iron.1.3 It is
4、assumed that the displacement cross section for ironis an adequate approximation for calculating displacements insteels that are mostly iron (95 to 100 %) in radiation fields forwhich secondary damage processes are not important.1.4 Procedures analogous to this one can be formulated forcalculating d
5、pa in charged particle irradiations. (See PracticeE521.)1.5 The application of this practice requires knowledge ofthe total neutron fluence and flux spectrum. Refer to PracticeE521 for determining these quantities.1.6 The correlation of radiation effects data is beyond thescope of this practice.1.7
6、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-bility of regulatory limitations prior to use.2. Referenced Docum
7、ents2.1 ASTM Standards:2E170 Terminology Relating to Radiation Measurements andDosimetryE521 Practice for Neutron Radiation Damage Simulationby Charged-Particle IrradiationE821 Practice for Measurement of Mechanical PropertiesDuring Charged-Particle IrradiationE853 Practice for Analysis and Interpre
8、tation of Light-Water Reactor Surveillance Results, E706(IA)3. Terminology3.1 Definitions for terms used in this practice can be foundin Terminology E170.4. Significance and Use4.1 A pressure vessel surveillance program requires a meth-odology for relating radiation-induced changes in materialsexpos
9、ed in accelerated surveillance locations to the conditionof the pressure vessel (see Practice E853). An importantconsideration is that the irradiation exposures be expressed ina unit that is physically related to the damage mechanisms.4.2 Amajor source of neutron radiation damage in metals isthe dis
10、placement of atoms from their normal lattice sites.Hence, an appropriate damage exposure index is the number oftimes, on the average, that an atom has been displaced duringan irradiation. This can be expressed as the total number ofdisplaced atoms per unit volume, per unit mass, or per atom ofthe ma
11、terial. Displacements per atom is the most common wayof expressing this quantity. The number of dpa associated witha particular irradiation depends on the amount of energydeposited in the material by the neutrons, and hence, dependson the neutron spectrum. (For a more extended discussion, seePractic
12、e E521.)4.3 No simple correspondence exists in general between dpaand a particular change in a material property. A reasonablestarting point, however, for relative correlations of propertychanges produced in different neutron spectra is the dpa valueassociated with each environment. That is, the dpa
13、 valuesthemselves provide a spectrum-sensitive index that may be auseful correlation parameter, or some function of the dpavalues may affect correlation.1This practice is under the jurisdiction of ASTM Committee E10 on NuclearTechnology and Applications and is the direct responsibility of Subcommitt
14、eeE10.05 on Nuclear Radiation Metrology.Current edition approved June 1, 2012. Published June 2012. Originallyapproved in 1979. Last previous edition approved in 2007 as E693 01(2007). DOI:10.1520/E0693-12.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer
15、Service at serviceastm.org. For Annual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.TABLE 1 ENDF/B-VI-based Iron Displacemen
16、t Cross SectionBin EngA(MeV) sd(barns) Bin EngA(MeV) sd(barns) Bin EngA(MeV) sd(barns)1 0.100E-09 158.3543 2 0.1050E-09 154.6209 3 0.110E-09 151.13954 0.1150E-09 147.8895 5 0.120E-09 144.1054 6 0.1275E-09 139.92027 0.1350E-09 136.0860 8 0.1425E-09 132.5445 9 0.150E-09 128.750210 0.160E-09 124.7860 1
17、1 0.170E-09 121.1728 12 0.180E-09 117.852713 0.190E-09 114.8137 14 0.200E-09 111.9561 15 0.210E-09 109.319916 0.220E-09 106.8646 17 0.230E-09 104.5694 18 0.240E-09 101.893019 0.2550E-09 98.93331 20 0.270E-09 96.65981 21 0.280E-09 94.1271722 0.300E-09 91.05218 23 0.320E-09 88.24872 24 0.340E-09 85.68
18、78725 0.360E-09 83.33912 26 0.380E-09 81.17265 27 0.400E-09 78.9247228 0.4250E-09 76.63646 29 0.450E-09 74.53734 30 0.4750E-09 72.5993031 0.500E-09 70.81827 32 0.5250E-09 69.14790 33 0.550E-09 67.5922234 0.5750E-09 66.13822 35 0.600E-09 64.64189 36 0.630E-09 63.1203937 0.660E-09 61.70157 38 0.690E-0
19、9 60.37332 39 0.720E-09 58.9273240 0.760E-09 57.39681 41 0.800E-09 55.97892 42 0.840E-09 54.6598443 0.880E-09 53.43220 44 0.920E-09 52.28703 45 0.960E-09 51.2154546 0.100E-08 50.07727 47 0.1050E-08 48.89598 48 0.110E-08 47.7960949 0.1150E-08 46.76870 50 0.120E-08 45.57125 51 0.1275E-08 44.2500652 0.
20、1350E-08 43.03653 53 0.1425E-08 41.91761 54 0.150E-08 40.7170855 0.160E-08 39.46333 56 0.170E-08 38.32018 57 0.180E-08 37.2696858 0.190E-08 36.30967 59 0.200E-08 35.40710 60 0.210E-08 34.5739161 0.220E-08 33.79705 62 0.230E-08 33.06956 63 0.240E-08 32.2242464 0.2550E-08 31.28942 65 0.270E-08 30.5700
21、2 66 0.280E-08 29.7699967 0.300E-08 28.79791 68 0.320E-08 27.91048 69 0.340E-08 27.1013970 0.360E-08 26.35879 71 0.380E-08 25.67357 72 0.400E-08 24.9630973 0.4250E-08 24.23960 74 0.450E-08 23.57548 75 0.4750E-08 22.9626876 0.500E-08 22.39920 77 0.5250E-08 21.87094 78 0.550E-08 21.3798279 0.5750E-08
22、20.91994 80 0.600E-08 20.44705 81 0.630E-08 19.9650982 0.660E-08 19.51724 83 0.690E-08 19.09670 84 0.720E-08 18.6398485 0.760E-08 18.15581 86 0.800E-08 17.70708 87 0.840E-08 17.2904988 0.880E-08 16.90205 89 0.920E-08 16.54074 90 0.960E-08 16.2016691 0.100E-07 15.84242 92 0.1050E-07 15.46908 93 0.110
23、E-07 15.1209494 0.1150E-07 14.79594 95 0.120E-07 14.41855 96 0.1275E-07 14.0009597 0.13050E-07 13.61661 98 0.1425E-07 13.26338 99 0.150E-07 12.88403100 0.160E-07 12.48759 101 0.170E-07 12.12633 102 0.180E-07 11.79428103 0.190E-07 11.49039 104 0.200E-07 11.20760 105 0.210E-07 10.94298106 0.220E-07 10
24、.69745 107 0.230E-07 10.46804 108 0.240E-07 10.20132109 0.2550E-07 9.906717 110 0.270E-07 9.679449 111 0.280E-07 9.427035112 0.300E-07 9.118745 113 0.320E-07 8.838819 114 0.340E-07 8.582926115 0.360E-07 8.347962 116 0.380E-07 8.131618 117 0.400E-07 7.907534118 0.4250E-07 7.678809 119 0.450E-07 7.468
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