ASTM E1450-2003 Standard Test Method for Tension Testing of Structural Alloys in Liquid Helium《液氦中结构合金抗拉试验的标准试验方法》.pdf
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1、Designation: E 1450 03Standard Test Method forTension Testing of Structural Alloys in Liquid Helium1This standard is issued under the fixed designation E 1450; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the year of last revisi
2、on. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon (e) indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method describes procedures for the tensiontesting of structural alloys in liquid helium. The format issimilar to that
3、 of other ASTM tension test standards, but thecontents include modifications for cryogenic testing whichrequires special apparatus, smaller specimens, and concern forserrated yielding, adiabatic heating, and strain-rate effects.1.2 To conduct a tension test by this standard, the specimenin a cryosta
4、t is fully submerged in normal liquid helium (He I)and tested using crosshead displacement control at a nominalstrain rate of 103s1or less. Tests using force control or highstrain rates are not considered.1.3 This standard specifies methods for the measurement ofyield strength, tensile strength, elo
5、ngation, and reduction ofarea. The determination of the elastic modulus is treated in TestMethod E 111.NOTE 1The boiling point of normal liquid helium (He I) at sea levelis 4.2 K (269C or 452.1F or 7.6R). It decreases with geographicelevation and is 4.0 K (269.2C or 452.5F or 7.2R) at the NationalIn
6、stitute of Standards and Technology in Colorado, 1677 m (5500 ft)above sea level. In this standard the temperature is designated 4 K.1.4 Values stated in SI units are treated as primary. Valuesstated in U.S. customary units are treated as secondary.1.5 This standard does not purport to address all o
7、f 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. See Section 5.2. Referenced Documents2.1 ASTM Standards:A 370 Tes
8、t Methods and Definitions for Mechanical Testingof Steel Products2E4 Practices for Force Verification of Testing Machines3E6 Terminology Relating to Methods of Mechanical Test-ing3E8 Test Methods for Tension Testing of Metallic Materials3E8M Test Methods for Tension Testing of Metallic Mate-rials Me
9、tric3E29 Practice for Using Significant Digits in Test Data toDetermine Conformance with Specifications4E83 Practice for Verification and Classification of Exten-someter System3E 111 Test Method forYoungs Modulus, Tangent Modulus,and Chord Modulus3E 1012 Practice for Verification of Specimen Alignme
10、ntUnder Tensile Loading33. Terminology3.1 Definitions:3.1.1 The definitions of terms relating to tension testing thatappear in Terminology E6shall apply here. The definitions inthis section also apply.3.1.2 adiabatic heatingthe internal heating of a specimenresulting from tension testing under condi
11、tions such that theheat generated by plastic work cannot be quickly dissipated tothe surrounding cryogen.3.1.3 adjusted length of the reduced sectionthe length ofthe reduced section plus an amount calculated to compensatefor strain in the fillet region.3.1.4 axial strainthe average of the longitudin
12、al strainsmeasured at opposite or equally spaced surface locations on thesides of the longitudinal axis of symmetry of the specimen. Thelongitudinal strains are measured using two or more strain-sensing devices located at the mid-length of the reducedsection.3.1.5 bending strainthe difference betwee
13、n the strain atthe surface of the specimen and the axial strain (the bendingstrain varies around the circumference and along the reducedsection of the specimen).3.1.6 Dewara vacuum-insulated container for cryogenicfluids.3.1.7 discontinuous yielding stress, sithe peak stress atthe initiation of the
14、first measurable serration on the curve ofstress-versus-strain.3.1.7.1 DiscussionThe parameter siis a function of testvariables and is not a material constant.1This test method is under the jurisdiction of ASTM Committee E28 onMechanical Testing and is the direct responsibility of Subcommittee E28.0
15、4 onUniaxial Testing.Current edition approved August 10, 2003. Published September 2003. Origi-nally approved in 1992. Last previous edition approved in 1998 as E 1459 92(1998).2Annual Book of ASTM Standards, Vol 01.03.3Annual Book of ASTM Standards, Vol 03.01.4Annual Book of ASTM Standards, Vol 14.
16、02.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.3.1.8 gage lengththe original distance between gagemarks made on the specimen for determining elongation afterfracture.3.1.9 length of the reduced sectionthe distance betweenthe tang
17、ent points of the fillets that bound the reduced section.3.1.10 maximum bending strainthe largest value of bend-ing strain in the reduced section of the specimen.3.1.10.1 DiscussionMaximum bending strength is calcu-lated from strains measured at two, three, or more circumfer-ential positions, and at
18、 each of two different longitudinalpositions.3.1.11 reduced sectionsection in the central portion of thespecimen, which has a cross section smaller than the grippedends.3.1.12 tensile cryostata test apparatus for applying tensileforces to test specimens in cryogenic environments (Fig. 1).4. Signific
19、ance and Use4.1 Tension tests provide information on the strength andductility of materials under uniaxial tensile stresses. Thisinformation may be useful for alloy development, comparisonand selection of materials, and quality control. Under certaincircumstances, the information may also be useful
20、for design.4.2 The force-time and force-extension records for alloystested in liquid helium using displacement control are serrated(1).5Serrations are formed by repeated bursts of unstableplastic flow and arrests. The unstable plastic flow (discontinu-ous yielding) is a free-running process occurrin
21、g in localizedregions of the reduced section at higher than nominal rates ofstrain with internal specimen heating. Examples of serratedstress-strain curves for a typical austenitic stainless steel withdiscontinuous yielding are shown in Fig. 2.4.3 A constant specimen temperature cannot be maintained
22、at all times during tests in liquid helium. The specimentemperature at local regions in the reduced section risestemporarily above 4 K during each discontinuous yieldingevent (see Fig. 2), owing to adiabatic heat. The number ofevents and the magnitude of the associated drops in magnitudeof force are
23、 a function of the material composition and otherfactors such as specimen size and test speed. Typically, alteringthe mechanical test variables can modify but not eliminate thediscontinuous yielding (2-4). Therefore, tensile property mea-surements of alloys in liquid helium (especially tensilestreng
24、th, elongation, and reduction of area) lack the usualsignificance of property measurements at room temperaturewhere deformation is more nearly isothermal and discontinu-ous yielding typically does not occur.4.4 The stress-strain response of a material tested in liquidhelium depends on whether force
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