ASTM D945-2006 Standard Test Methods for Rubber Properties in Compression or Shear (Mechanical Oscillograph)《在压缩应力和剪切应力下橡胶特性的试验方法(机械示波器)》.pdf
《ASTM D945-2006 Standard Test Methods for Rubber Properties in Compression or Shear (Mechanical Oscillograph)《在压缩应力和剪切应力下橡胶特性的试验方法(机械示波器)》.pdf》由会员分享,可在线阅读,更多相关《ASTM D945-2006 Standard Test Methods for Rubber Properties in Compression or Shear (Mechanical Oscillograph)《在压缩应力和剪切应力下橡胶特性的试验方法(机械示波器)》.pdf(11页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: D 945 06Standard Test Methods forRubber Properties in Compression or Shear (MechanicalOscillograph)1This standard is issued under the fixed designation D 945; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the year of
2、 last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon (e) indicates an editorial change since the last revision or reapproval.This standard has been approved for use by agencies of the Department of Defense.1. Scope1.1 These test methods cover the use of
3、 the Yerzley me-chanical oscillograph for measuring mechanical properties ofrubber vulcanizates in the generally small range of deformationthat characterizes many technical applications. These proper-ties include resilience, dynamic modulus, static modulus,kinetic energy, creep, and set under a give
4、n force. Measure-ments in compression and shear are described.2,31.2 The test is applicable primarily, but not exclusively, tomaterials having static moduli at the test temperature such thatforces below 2 MPa (280 psi) in compression or 1 MPa(140 psi) in shear will produce 20 % deformation, and havi
5、ngresilience such that at least three complete cycles are producedwhen obtaining the damped oscillatory curve. The range maybe extended, however, by use of supplementary masses andrefined methods of analysis. Materials may be compared eitherunder comparable mean stress or mean strain conditions.1.3
6、The values stated in SI units are to be regarded as thestandard. The values given in parentheses are for informationonly.1.4 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-p
7、riate safety and health practices and determine the applica-bility of regulatory limitations prior to use. For a specificwarning see 12.14.2. Referenced Documents2.1 ASTM Standards:4D 832 Practice for Rubber Conditioning For Low Tempera-ture TestingD 1207 Recommended Practice for Classifying Elastom
8、ericCompounds for Resilient Automotive Mountings5D 4483 Practice for Evaluating Precision for Test MethodStandards in the Rubber and Carbon Black ManufacturingIndustries2.2 SAE Standard:SAE J16 Classification of Elastomer Compounds for Auto-motive Resilient Mountings6,73. Terminology3.1 Descriptions
9、 of Terms Specific to This Standard:3.2 effective dynamic moduluscalculated from the for-mula for simple harmonic motion in a damped free oscillation.It is a composite index which includes the effect of suchdiverse factors as nonlinearity of stress-strain, changing mo-lecular energies, and heat loss
10、es.3.3 point modulusratio of total stress (force/area) to totalstrain (change in dimension/unstressed dimension) at one pointof the stress-strain curve. Sometimes called the “secant modu-lus,” it is equal to the slope of a line from the origin to thechosen point.3.4 static modulussynonymous with “ta
11、ngent modulus”and is the slope of the tangent to the stress-strain curve at a1These test methods are under the jurisdiction of ASTM Committee D11 onRubber and are the direct responsibility of Subcommittee D11.14 on Time andTemperature-Dependent Physical Properties.Current edition approved July 1, 20
12、06. Published July 2006. Originally approvedin 1948. Last previous edition approved in 2001 as D 945 92 (2001)e1.2A survey of some aspects of hysteresis and modulus in dynamic performanceof polymers is available in a paper by Payne, A. R., “The Role of Hysteresis inPolymers,” Rubber Journal, January
13、 1964, p. 36.3One method of correlating fundamental data from theYerzley oscillograph withdynamic tests at constant amplitude is described by Baldwin, F. P., in his paper,“Determination of the Dynamic Properties of Rubberlike Materials by Means of aModified Yerzley Oscillograph,” The Rubber Age, Apr
14、il 1950.4For referenced ASTM 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.5Withdrawn.6Available from Society of Automotive Engi
15、neers, 400 Commonwealth Drive,Warrendale, PA 15096.7The Yerzley oscillograph was originally described in detail in the paper byYerzley, F. L., “A Mechanical Oscillograph for Routine Tests of Rubber andRubber-Like Materials,” Proceedings, ASTM, Vol 39, 1939, p. 1180; also RubberChemistry and Technolo
16、gy, Vol XIII, No. 1, January 1940, p. 149.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.chosen point. It can provide a reference for comparison withthe effective dynamic modulus at that point.4. Summary of Test Methods4.1 Specimens
17、 are loaded by an unbalanced lever and theresultant deflections are recorded on a chronograph. Thispermits calculations to be made of static modulus at any stageof a stepwise loading or unloading schedule. Creep andrecovery rates, including set under prescribed conditions, canbe obtained. Since the
18、lever is supported on a knife edge, thesystem can be impact-loaded to produce a damped freeoscillation trace. This trace yields a dynamic modulus, aresilience index, an oscillation frequency, and a measurementof stored energy.5. Significance and Use5.1 The rubber properties that are measurable by th
19、ese testmethods are important for the isolation and absorption of shockand vibration.These properties may be used for quality control,development and research.5.2 Measurements in compression are influenced by speci-men shape. This shape factor may be described as the ratio ofthe loaded surface area
20、to the unloaded surface area. Inapplying data from a compression specimen, shape factor mustbe incorporated into the mathematical transferal to the appli-cation.6. Apparatus6.1 The essential features of the apparatus7,8(illustrated inFig. 1 and Fig. 2) are as follows:6.1.1 The beam shall be supporte
21、d at its center by aknife-edge, A, and shall be so designed that a test specimenplaced beneath the micrometer can be loaded by placingstandard masses alternatively on front and back portions of thecross-rod, F, at the pen end of the beam. A second knife-edge,B, and a stabilizing arm, B8, (as shown i
22、n Fig. 2), shall be usedto apply load to the test specimen and to maintain parallelismof the loading platens. Optional knife-edges, C and D, may beused to extend the range of the oscillograph.6.1.2 Apen shall extend lengthwise from the beam to recorddeflections on the oscillogram automatically. From
23、 Fig. 2,itisapparent that the deflection of the specimen under test will bemagnified by the travel of the pen in proportion to the leverratio which will be 10:1 when the sample is on the inner testposition, B. Therefore, a deformation of 2.5 mm, for example,will be registered on the oscillogram as a
24、 vertical displacementof 25 mm.6.1.3 The masses, MF,MG, and MH, derive from the mass ofaccurately machined disks, 99.06 mm in diameter with a8The sole source of supply of the Yerzley oscillograph known to the committeeat this time is Tavdi Co., Inc., P.O. Box 298, Barrington, RI 02806. If you are aw
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