ASTM E693-2017 9375 Standard Practice for Characterizing Neutron Exposures in Iron and Low Alloy Steels in Terms of Displacements Per Atom (DPA)《根据每个原子(DPA)位移辨别铁和低合金钢中子照射特性的标准实施规程》.pdf
《ASTM E693-2017 9375 Standard Practice for Characterizing Neutron Exposures in Iron and Low Alloy Steels in Terms of Displacements Per Atom (DPA)《根据每个原子(DPA)位移辨别铁和低合金钢中子照射特性的标准实施规程》.pdf》由会员分享,可在线阅读,更多相关《ASTM E693-2017 9375 Standard Practice for Characterizing Neutron Exposures in Iron and Low Alloy Steels in Terms of Displacements Per Atom (DPA)《根据每个原子(DPA)位移辨别铁和低合金钢中子照射特性的标准实施规程》.pdf(8页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E693 17Standard Practice forCharacterizing Neutron Exposures in Iron and Low AlloySteels in Terms of Displacements Per Atom (DPA)1This standard is issued under the fixed designation E693; the number immediately following the designation indicates the year oforiginal adoption or, in the
2、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 irradiations of
3、 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 d(E) is known(see Practice E521), this practice is written specifically for iron.1.3 It is assumed tha
4、t 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 dpa in charg
5、ed 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 This standa
6、rd 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, health, and environmental practices and deter-mine the applicability of regulatory limitations prior to use.1.8 This inter
7、national standard was developed in accor-dance with internationally recognized principles on standard-ization established in the Decision on Principles for theDevelopment of International Standards, Guides and Recom-mendations issued by the World Trade Organization TechnicalBarriers to Trade (TBT) C
8、ommittee.2. Referenced Documents2.1 ASTM Standards:2E170 Terminology Relating to Radiation Measurements andDosimetryE521 Practice for Investigating the Effects of Neutron Ra-diation Damage Using Charged-Particle IrradiationE821 Practice for Measurement of Mechanical PropertiesDuring Charged-Particle
9、 IrradiationE853 Practice for Analysis and Interpretation of Light-WaterReactor Surveillance Results3. 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 rad
10、iation-induced changes in materialsexposed 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 A major source of neu
11、tron radiation damage in metals isthe displacement 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 vo
12、lume, per unit mass, or per atom ofthe material. 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. (F
13、or a more extended discussion, seePractice 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 property1This practice is under the jurisdiction of ASTM Committee E10 on Nucle
14、arTechnology and Applicationsand is the direct responsibility of SubcommitteeE10.05 on Nuclear Radiation Metrology.Current edition approved Aug. 1, 2017. Published September 2017. Originallyapproved in 1979. Last previous edition approved in 2012 as E693 121. DOI:10.1520/E0693-17.2For referenced AST
15、M 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.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohoc
16、ken, PA 19428-2959. United StatesThis international standard was developed in accordance with internationally recognized principles on standardization established in the Decision on Principles for theDevelopment of International Standards, Guides and Recommendations issued by the World Trade Organiz
17、ation Technical Barriers to Trade (TBT) Committee.1changes produced in different neutron spectra is the dpa valueassociated with each environment. That is, the dpa valuesthemselves provide a spectrum-sensitive index that may be auseful correlation parameter, or some function of the dpavalues may aff
18、ect correlation.TABLE 1 ENDF/B-VI-based Iron Displacement Cross SectionBin EngA(MeV) d(barns) Bin EngA(MeV) d(barns) Bin EngA(MeV) d(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
19、 132.5445 9 0.150E-09 128.750210 0.160E-09 124.7860 11 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
20、-09 91.05218 23 0.320E-09 88.24872 24 0.340E-09 85.6878725 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 3
21、6 0.630E-09 63.1203937 0.660E-09 61.70157 38 0.690E-09 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 46.76
22、870 50 0.120E-08 45.57125 51 0.1275E-08 44.2500652 0.1350E-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-0
23、8 32.2242464 0.2550E-08 31.28942 65 0.270E-08 30.57002 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.
24、5250E-08 21.87094 78 0.550E-08 21.3798279 0.5750E-08 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 16.20166
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