ASTM D5099-2008 Standard Test Methods for Rubber&x2014 Measurement of Processing Properties Using Capillary Rheometry《使用毛细管流变仪对橡胶加工性能的标准试验方法》.pdf
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1、Designation: D 5099 08Standard Test Methods forRubberMeasurement of Processing Properties UsingCapillary Rheometry1This standard is issued under the fixed designation D 5099; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, the year
2、 of 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.1. Scope1.1 These test methods describe how capillary rheometrymay be used to measure the rheological characteristics ofrubbe
3、r (raw or compounded). Two methods are addressed:Method Ausing a piston type capillary rheometer, andMethod Busing a screw extrusion type capillary rheometer.The two methods have important differences, as outlined in7-10 and 11-14, respectively.1.2 These test methods cover the use of a capillary rhe
4、om-eter for the measurement of the flow properties of thermoplas-tic elastomers, unvulcanized rubber, and rubber compounds.These material properties are related to factory processing.1.3 Since piston type capillary rheometers impart only asmall amount of shearing energy to the sample, these measure-
5、ments directly relate to the state of the compound at the time ofsampling. Piston type capillary rheometer measurements willusually differ from measurements with a screw extrusion typerheometer, which imparts shearing energy just before therheological measurement.1.4 Capillary rheometer measurements
6、 for plastics are de-scribed in Test Method D 3835.1.5 The values stated in SI units are to be regarded asstandard. The values given in parentheses are for informationonly.1.6 This standard does not purport to address all of thesafety concerns, if any, associated with its use. It is theresponsibilit
7、y 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:2D 1349 Practice for RubberStandard Temperatures forTestingD 1418 Practice for Rubber and Rubber Lati
8、cesNomenclatureD 1485 Practice for Rubber from Natural SourcesSampling and Sample PreparationD 3182 Practice for RubberMaterials, Equipment, andProcedures for Mixing Standard Compounds and Prepar-ing Standard Vulcanized SheetsD 3835 Test Method for Determination of Properties ofPolymeric Materials b
9、y Means of a Capillary RheometerD 3896 Practice for Rubber From Synthetic SourcesSamplingD 4483 Practice for Evaluating Precision for Test MethodStandards in the Rubber and Carbon Black ManufacturingIndustries3. Terminology3.1 Definitions of Terms Specific to This Standard:3.1.1 The following terms
10、appear in logical order for thesake of clarity:3.1.2 capillary rheometeran instrument in which rubbercan be forced from a reservoir through a capillary die; thetemperature, pressure entering the die, and flow rate throughthe die can be controlled and accurately measured.3.1.3 die entrance pressure (
11、P)the pressure in the reser-voir at the die entrance, in Pa.3.1.4 volumetric flow rate (Q)the flow rate through thecapillary die, in mm3/s.3.1.5 apparent (uncorrected) shear rate (ga)shear strainrate (or velocity gradient) of the rubber extrudate as it passesthrough the capillary die (Eq 1), in s1.3
12、.1.5.1 DiscussionThis velocity gradient is not uniformthrough the cross-section of the capillary die. The shear rate iscalculated for the region of highest shear, at the wall of thecapillary. By selecting a die diameter and controlling thevolumetric flow rate (Q) through the die, a specific level of
13、apparent shear rate may be achieved. Alternately, the shearstress (die entrance pressure, P) may be controlled, and theapparent shear rate measured.Mathematically, the apparent shear rate for a Newtonianfluid at the wall is given as follows:ga532 Qp D3(1)1These test methods are under the jurisdictio
14、n of ASTM Committee D11 onRubber and are the direct responsibility of Subcommittee D11.12 on ProcessabilityTests.Current edition approved May 1, 2008. Published May 2008. Originallyapproved in 1993. Last previous edition approved in 2003 as D 5099 93 (2003).2For referenced ASTM standards, visit the
15、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.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, Un
16、ited States.where:ga= apparent shear rate, s1,Q = volumetric flow rate, mm3/s,p = the constant pi, approximately 3.142, andD = diameter of the capillary die, mm.3.1.6 apparent shear stress (ta)the measured resistance toflow through a capillary die (Eq 2).ta5P4L/D!(2)where:ta= apparent shear stress,
17、Pa,P = pressure at the entrance to the capillary die, Pa,L = length of the capillary die, mm, andD = diameter of the capillary die, mm.3.1.7 apparent viscosity (ha)ratio of apparent shear stressto apparent shear rate, in Pa-s.3.1.7.1 DiscussionFor a capillary rheometer, the apparentviscosity is usua
18、lly calculated at a given shear rate.At constanttemperature, the apparent viscosity of most polymers is notconstant, but varies with shear rate. The viscosity is generallyannotated with the shear rate at which the measurement wasmade.3.1.8 Newtonian fluida fluid for which viscosity does notvary with
19、 changing shear rate. Simple liquids such as rubberextender oils are Newtonian; most polymeric materials are not.3.1.9 power law fluida fluid material for which theviscosity varies with the shear rate in accordance with therelationship:t5Kg!N(3)where:K = constant, often called consistency index, and
20、N = a material parameter generally called the power lawindex. It is equal to 1.0 for Newtonian fluids andgenerally between 0.18 and 0.33 for compoundedrubbers or elastomers, or both, with some exceptions.Most non-Newtonian fluids follow the relationship in Eq 3for at least short ranges of the shear
21、rate variable. Eq 3 isgenerally used in its logarithmic form, as:logt! 5 log K! 1 N log g! (4)3.1.10 corrected shear stress (tw)the shear stress at thewall of the capillary die; it is calculated from the apparent shearstress by applying the Bagley correction E in Eq. 5 for energylosses at the entran
22、ce and exit of the die.3.1.10.1 DiscussionThe Bagley correction, often termed“end effect,” is normally applied as though it were an addi-tional length of capillary, in terms of an added L/D ratio. TheCapillary entrance angle and geometry have great influence onthe magnitude of this correction.3.1.10
23、.2 DiscussionSince the magnitude of the Bagleycorrection is a function of shear rate, data for this correction areobtained by using two or more dies of different lengths butpreferably of the same diameter and volumetric flow rate (andthus the same apparent shear rate). If the data from theseaddition
24、al dies are compared, either graphically or mathemati-cally, a linear relationship of extrusion pressure with diegeometry is usually obtained, of the following form:P 5 cFLD1 EG(5)where:c = slope of the line, andE = Bagley correction, expressed as the negative capillarylength to diameter (L/D) ratio
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