ASTM E646-2016 red 5782 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 E646-2016 red 5782 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 E646-2016 red 5782 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(13页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E646 15E646 16Standard 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.INTRODUCTIONThis test method for determining tensile strain-hardening exponents n utilizes stress-stain dataobtained i
3、n 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 interest of the true-stress versus true-strain curve. Themathematical rep
4、resentation used in this method is a power curve (Note 1) of the form (1)2: = Knwhere: = true stress, = plastic component of true strain, but in special cases may be the total true strain. (See 10.2),K = is a constant, often called the strength coefficient having the units of stress, andn = strain-h
5、ardening exponent1. Scope Scope*1.1 This test method covers the determination of a strain-hardening exponent by tension testing of metallic sheet materials forwhich plastic-flow behavior obeys the power curve given in the Introduction.NOTE 1A single power curve may not be a satisfactory fit to the e
6、ntire stress-strain curve between yield and necking. If such is the case, more thanone value of the strain-hardening exponent may be obtained (2) by agreement using this test method.1.2 This test method is specifically for metallic sheet materials with thicknesses of at least 0.005 in. (0.13 mm) but
7、 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 to be regarded as standard. The values given in parentheses are mathematicalconversions to SI units that are provided for i
8、nformation only and are not considered standard.NOTE 2The value of the strain-hardening exponent, n, is has no units and 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 responsib
9、ilityof the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatorylimitations prior to use.2. Referenced Documents2.1 ASTM Standards:3E4 Practices for Force Verification of Testing MachinesE6 Terminology Relating to Methods of Mechani
10、cal TestingE8/E8M Test Methods for Tension 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
11、 Chord Modulus1 This test method is under the jurisdiction of ASTM Committee E28 on Mechanical Testing and is the direct responsibility of Subcommittee E28.02 on Ductility andFormability.Current edition approved Nov. 15, 2015Feb. 1, 2016. Published February 2016March 2016. Originally approved in 197
12、8. Last previous edition approved in 20072015 asE646 - 07E646 - 15.1. DOI: 10.1520/E0646-15.10.1520/E0646-162 The boldface numbers 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 Servi
13、ce at serviceastm.org. For Annual Book of ASTM Standardsvolume information, refer to the standards Document Summary page on the 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
14、 version. Becauseit may not be technically possible to adequately depict all changes accurately, ASTM recommends that users consult prior editions as appropriate. In all cases only the current versionof the standard as published by ASTM is to be considered the official document.*A Summary of Changes
15、 section appears at the end of this standardCopyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States1E177 Practice for Use of the Terms Precision and Bias in ASTM Test MethodsE691 Practice for Conducting an Interlaboratory Study to Determine t
16、he 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 other terms used in this test method, refer to E6 (Standard Terminology Relating to Methods ofMechanical Testing).
17、3.2 Definitions:3.2.1 elastic true strain, e, nelastic component of the true strain.3.2.2 engineering strain, e, na dimensionless value that is the change in length (L) per unit length of original lineardimension (L0) along the loading axis of the specimen; that is, e = L/L0.3.2.3 engineering stress
18、, S FL-2 , nthe normal stress, expressed in units of applied force, F per unit of originalcross-sectional area, A0; that is, S = F/A03.2.4 necking, nthe onset of nonuniform or localized plastic deformation, resulting in a localized reduction of cross-sectionalarea.3.2.5 plastic true strain, p, nthe
19、inelastic component of true strain.3.2.6 strain hardening, nan increase in hardness and strength caused by plastic deformation.3.2.7 true strain, , nthe natural logarithm of the ratio of instantaneous gauge length, L, to the original gauge length, L0; thatis, = ln (L/L0) or = ln (1+e).3.2.8 true str
20、ess, FL-2 , nthe instantaneous normal stress, calculated on the basis of the instantaneous cross-sectional area,A; that is, = F/A; if no necking has occurred , occurred, = S(1+e).3.3 Definitions of Terms Specific to This Standard:3.3.1 strain-hardening exponent (n), nan experimental constant, comput
21、ed from the least 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 th
22、e data to the assumed 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
23、a continuous and rate-controlled manner while the normal tensile load and strain are monitored. Theinstantaneous cross-sectional area may be monitored or calculated by assuming constancy of volume in the plastic region.Equations are presented that permit the calculation of the true stress, , true st
24、rain, , strain-hardening exponent, n, and strengthcoefficient, K, for that continuous portion of the true-stress versus true-strain curve which follows the empirical relationshipsdescribed.NOTE 3This test method is recommended for use only in the plastic range for metallic sheet material for which t
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