ASTM D6204-2015 3064 Standard Test Method for Rubber&x2014 Measurement of Unvulcanized Rheological Properties Using Rotorless Shear Rheometers《橡胶的标准试验方法 采用无转子剪切流变仪测量橡胶未硫化流变特性》.pdf
《ASTM D6204-2015 3064 Standard Test Method for Rubber&x2014 Measurement of Unvulcanized Rheological Properties Using Rotorless Shear Rheometers《橡胶的标准试验方法 采用无转子剪切流变仪测量橡胶未硫化流变特性》.pdf》由会员分享,可在线阅读,更多相关《ASTM D6204-2015 3064 Standard Test Method for Rubber&x2014 Measurement of Unvulcanized Rheological Properties Using Rotorless Shear Rheometers《橡胶的标准试验方法 采用无转子剪切流变仪测量橡胶未硫化流变特性》.pdf(12页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: D6204 15Standard Test Method forRubberMeasurement of Unvulcanized RheologicalProperties Using Rotorless Shear Rheometers1This standard is issued under the fixed designation D6204; the number immediately following the designation indicates the year oforiginal adoption or, in the case of
2、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 test method covers the use of a rotorless oscillatingshear rheometer for the measurement of
3、 the flow properties ofraw rubber and unvulcanized rubber compounds. These flowproperties are related to factory processing.1.2 The values stated in SI units are to be regarded asstandard. The values given in parentheses are for informationonly.1.3 This standard does not purport to address all of th
4、esafety 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.2. Referenced Documents2.1 ASTM Standards:2D1485 Practice for Rubber f
5、rom Natural SourcesSampling and Sample PreparationD1646 Test Methods for RubberViscosity, StressRelaxation, and Pre-Vulcanization Characteristics(Mooney Viscometer)D3896 Practice for Rubber From Synthetic SourcesSamplingD4483 Practice for Evaluating Precision for Test MethodStandards in the Rubber a
6、nd Carbon Black ManufacturingIndustriesD5289 Test Method for Rubber PropertyVulcanizationUsing Rotorless Cure MetersD6601 Test Method for Rubber PropertiesMeasurementof Cure and After-Cure Dynamic Properties Using aRotorless Shear Rheometer3. Terminology3.1 Definitions of Terms Specific to This Stan
7、dard:3.1.1 complex shear modulus, G*, nthe ratio of peakamplitude shear stress to peak amplitude shear strain;mathematically, G*=(S*/Area )/Strain=(G2+ G”2)1/2.3.1.2 complex torque, S*, nthe peak amplitude torqueresponse measured by a reaction torque transducer for asinusoidally applied strain; math
8、ematically, S* is computed byS*=(S2+ S”2)1/2.3.1.3 dynamic complex viscosity *, nthe ratio of thecomplex shear modulus, G* to the oscillation frequency, ,inradians per second.3.1.4 elastic torque, S, nthe peak amplitude torque com-ponent that is in phase with a sinusoidally applied strain.3.1.5 loss
9、 angle, ,nthe phase angle by which thecomplex torque (S*) leads a sinusoidally applied strain.3.1.6 loss factor, tan ,nthe ratio of loss modulus tostorage modulus, or the ratio of viscous torque to elastictorque; mathematically, tan = G”/G = S”/S.3.1.7 loss shear modulus G”, nthe ratio of (viscous)
10、peakamplitude shear stress to peak amplitude shear strain for thetorque component 90 out of phase with a sinusoidally appliedstrain; mathematically, G” =(S”/Area)/Peak Strain.3.1.8 real dynamic viscosity, ,nthe ratio of the loss shearmodulus, G” to the oscillation frequency, , in radians persecond.3
11、.1.9 storage shear modulus, G, nthe ratio of (elastic)peak amplitude shear stress to peak amplitude shear strain forthe torque component in phase with a sinusoidally appliedstrain; mathematically, G=(S/Area)/Peak Strain.3.1.10 viscous torque, S”, nthe peak amplitude torquecomponent, which is 90 out
12、of phase with a sinusoidallyapplied strain.4. Summary of Test Method4.1 A rubber test specimen is contained in a die cavity thatis closed and maintained at an elevated temperature. The cavityis formed by two dies, one of which is oscillated through arotary amplitude. This action produces a sinusoida
13、l torsionalstrain in the test specimen, resulting in a sinusoidal torque,which measures a viscoelastic quality of the test specimen. The1This test method is under the jurisdiction of ASTM Committee D11 on Rubberand is the direct responsibility of Subcommittee D11.12 on Processability Tests.Current e
14、dition approved Nov. 1, 2015. Published December 2015. Originallyapproved in 1997. Last previous edition approved in 2012 as D6204 12. DOI:10.1520/D6204-15.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of AST
15、MStandards volume information, refer to the standards Document Summary page onthe ASTM website.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States1test specimen can be either a raw natural or synthetic rubber oran uncured rubber compound.
16、4.2 These viscoelastic measurements can be made based on(1) a frequency sweep, in which the frequency is programmedto change in steps under constant strain amplitude and tem-perature conditions, (2) a strain sweep, in which the strainamplitude is programmed to change in steps under constantfrequency
17、 and temperature conditions, or (3) a temperaturesweep, in which the temperature is programmed to eitherincrease or decrease under constant strain amplitude andfrequency conditions. A timed test may also be performed inwhich a sinusoidal strain is applied for a given time periodunder constant strain
18、 amplitude, frequency, and temperatureconditions.4.2.1 For a frequency sweep test, the instrument is typicallyprogrammed to increase the frequency with each subsequentstep change. For a strain sweep test, the instrument is usuallyprogrammed to increase the strain amplitude with each subse-quent step
19、 change. This is done to minimize the influence ofprior test conditions on subsequent test steps. For temperaturesweeps, the temperature may be programmed either to increaseor decrease with each subsequent step change, depending onthe effects to be studied. The results from increasing frequency,stra
20、in amplitude, or temperature may not be the same as resultsfrom decreasing these test parameters.4.3 Rheological properties are measured for each set offrequency, strain, and temperature conditions. These propertiescan be measured as combinations of elastic torque S, viscoustorque S”, storage shear
21、modulus G, loss shear modulus G”,tan , complex dynamic viscosity *, and real dynamicviscosity .4.4 This standard is organized in three different parts (A, B,and C), which can be run in the following combinations:ABA, BA, B, CA, CB, CC4.5 These three parts are described below:4.5.1 Part A is a rapid
22、three-point frequency sweep per-formed at a low strain of 7 % to relate to differences in averagemolecular weight, molecular weight distribution, and longchain branching for raw elastomers and to relate to differencesin flowability, shear thinning, and die swell for mixed batches.4.5.2 Part B is a r
23、apid two-point frequency sweep performedat a moderate strain of 100 % (or higher) to relate to geldifferences with raw elastomers and to relate to differences inhigher shear rate viscosity and die swell for mixed batches. Thehigher applied strain is commonly needed to help break up gelstructure in s
24、ome raw elastomers and break up filler aggregatenetworks for mixed batches.Although 100 % strain is the morecommon test condition, significantly higher test sensitivity ispossible by performing this frequency sweep at 200 % strain orhigher.4.5.3 Part C is a linear ramped temperature rise fromprocess
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