ASTM E646-2015 red 1556 Standard Test Method for Tensile Strain-Hardening Exponents (n -Values) of Metallic Sheet Materials《金属薄板材拉伸应变硬化指数 (n值) 的标准试验方法》.pdf
《ASTM E646-2015 red 1556 Standard Test Method for Tensile Strain-Hardening Exponents (n -Values) of Metallic Sheet Materials《金属薄板材拉伸应变硬化指数 (n值) 的标准试验方法》.pdf》由会员分享,可在线阅读,更多相关《ASTM E646-2015 red 1556 Standard Test Method for Tensile Strain-Hardening Exponents (n -Values) of Metallic Sheet Materials《金属薄板材拉伸应变硬化指数 (n值) 的标准试验方法》.pdf(11页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E646 071E646 15Standard Test Method forTensile Strain-Hardening Exponents (n -Values) of MetallicSheet Materials1This standard is issued under the fixed designation E646; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision,
2、 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 NOTEThe equation in 10.3 was editorially corrected in January 2014.INTRODUCTIONThis test method for determining ten
3、sile strain-hardening exponents n utilizes stress-stain dataobtained in a uniaxial tension test. Tensile data are obtained in a continuous and rate-controlledmanner via displacement or strain control. The strain-hardening exponents are determined from anempirical representation over the range of int
4、erest of the true-stress versus true-strain curve. Themathematical representation used in this method is a power curve (Note 1) of the form (1)2: = Knwhere: = true stress, = true plastic strain, = plastic component of true strain, but in special cases may be the total true strain. (See 10.2),K = str
5、ength coefficient, andK = is a constant, often called the strength coefficient having the units of stress, andn = strain-hardening exponent1. Scope1.1 This test method covers the determination of a strain-hardening exponent by tension testing of metallic sheet materials forwhich plastic-flow behavio
6、r obeys the power curve given in the Introduction.NOTE 1A single power curve may not fit be a satisfactory fit to the entire stress-strain curve between yield and necking. If such is the case, morethan one value of the strain-hardening exponent canmay be obtained (2).) by agreement using this test m
7、ethod.1.2 This test method is specifically for metallic sheet materials with thicknesses of at least 0.005 in. (0.13 mm) but not greaterthan 0.25 in. (6.4 mm). The method has successfully been and may be applied to other forms and thicknesses by agreement1.3 The values stated in inch-pound units are
8、 to be regarded as the standard. The SI equivalents shown may beapproximate.standard. The values given in parentheses are mathematical conversions to SI units that are provided for informationonly and are not considered standard.NOTE 2The value of the strain-hardening exponent, n, is has no units an
9、d is independent of the units used in its determination1.4 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibilityof the user of this standard to establish appropriate safety and health practices and determine the applicability
10、of regulatorylimitations prior to use.2. Referenced Documents2.1 ASTM Standards:3E4 Practices for Force Verification of Testing MachinesE6 Terminology Relating to Methods of Mechanical Testing1 This test method is under the jurisdiction of ASTM Committee E28 on Mechanical Testing and is the direct r
11、esponsibility of Subcommittee E28.02 on Ductility andFormability.Current edition approved Nov. 15, 2015. Published December 2007February 2016. Originally approved in 1978. Last previous edition approved in 20002007 asE646 - 00.E646 - 071. DOI: 10.1520/E0646-07E01.10.1520/E0646-15.2 The boldface numb
12、ers in parentheses refer to the list of references appended to this method.3 For referencedASTM standards, visit theASTM website, www.astm.org, or contactASTM Customer Service at serviceastm.org. For Annual Book of ASTM Standardsvolume information, refer to the standards Document Summary page on the
13、 ASTM website.This document is not an ASTM standard and is intended only to provide the user of an ASTM standard an indication of what changes have been made to the previous version. Becauseit may not be technically possible to adequately depict all changes accurately, ASTM recommends that users con
14、sult prior editions as appropriate. In all cases only the current versionof the standard as published by ASTM is to be considered the official document.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States1E8E8/E8M Test Methods for Tension
15、Testing of Metallic MaterialsE29 Practice for Using Significant Digits in Test Data to Determine Conformance with SpecificationsE83 Practice for Verification and Classification of Extensometer SystemsE111 Test Method for Youngs Modulus, Tangent Modulus, and Chord ModulusE177 Practice for Use of the
16、Terms Precision and Bias in ASTM Test MethodsE691 Practice for Conducting an Interlaboratory Study to Determine the Precision of a Test Method2.2 ISO StandardISO 10275:2007 Metallic materials - Sheet and strip - Determination of tensile strain hardening exponent3. Terminology3.1 For definitions of o
17、ther terms used in this test method, refer to E6 (Standard Terminology Relating to Methods ofMechanical Testing).3.2 Definitions:3.1.1 The definitions of terms given in Terminology E6 shall apply, with the addition of the following special terms used in thismethod.3.2.1 elastic true strain, e, nelas
18、tic component of the true strain.3.2.2 engineering strain (e)strain, e, na dimensionless value that is the change in length (LL) per unit length of originallinear dimension (L0) along the loading axis of the specimen; that is, e = e = (L)L/LL0.3.2.3 engineering stress (S)stress, S FLFL2-2 , nthe nor
19、mal stress, expressed in units of applied force, F,F per unit oforiginal cross-sectional area, A0; that is, S = FS = AF/A0.3.2.4 neckingnecking, nthe onset of nonuniform or localized plastic deformation, resulting in a localized reduction ofcross-sectional area.3.2.5 plastic true strain, p, nthe ine
20、lastic component of true strain.3.2.6 strain-hardening (n)strain hardening, nan increase in hardness and strength caused by plastic deformation.3.1.6 strength coeffcient (K) FL2an experimental constant, computed from the fit of the data to the assumed power curve,that is numerically equal to the ext
21、rapolated value of true stress at a true strain of 1.00.3.2.7 true strain ()strain, , nthe natural logarithm of the ratio of instantaneous gagegauge length, L, to the originalgagegauge length, L00; that is, = 1n = ln (L L/L L0) or = 1n = ln (1+e).3.2.8 true stress ()stress, FLFL2-2 , nthe instantane
22、ous normal stress, calculated on the basis of the instantaneouscross-sectional area, A; that is, = = F/A; if no necking has occurred, = occurred , = S( S(1+e).1+e).3.3 Definitions of Terms Specific to This Standard:3.3.1 strain-hardening exponent (n), nan experimental constant, computed from the lea
23、st squares best fit, linear slope of log versus log or data over a specific strain range where is the plastic component of true strain, but in special cases may be thetotal true strain (see 10.2).3.3.2 strength coeffcient (K) FL2, nan experimental constant, computed from the fit of the data to the a
24、ssumed powercurve, that is numerically equal to the extrapolated value of true stress at a true strain of 1.00.4. Summary of Test Method4.1 This test method applies to materials exhibiting a continuous stress-strain curve in the plastic region. The displacement orstrain is applied in a continuous an
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