ASTM D5099-1993(2003) Standard Test Methods for Rubber-Measurement of Processing Properties Using Capillary Rheometry《使用毛细管流变仪对橡胶加工性能的测试方法》.pdf
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1、Designation: D 5099 93 (Reapproved 2003)Standard 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
2、revision, the year 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 chara
3、cteristics ofrubber (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
4、of a capillary rheom-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 samp
5、le, these measure-ments directly relate to the state of the compound at the time ofsampling. Piston capillary rheometer measurements will usu-ally differ from measurements with a screw extrusion typerheometer, which imparts shearing energy just before therheological measurement.1.4 Capillary rheomet
6、er measurements 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 t
7、heresponsibility 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 1485 Test Methods for Rub
8、ber 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 by Means of a Capillary RheometerD 3896
9、 Practice for Rubber from Synthetic SourcesSamplingD 4483 Practice for Determining Precision for Test MethodStandards in the Rubber and Carbon Black Industries3. Terminology3.1 Definitions of Terms Specific to This Standard:3.1.1 apparent (uncorrected) shear rate (g)shear strainrate (or velocity gra
10、dient) of the rubber extrudate as it passesthrough the capillary die.3.1.1.1 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 contro
11、lling thevolume flow per unit time through the die, a specific level ofapparent shear rate may be achieved. Alternately, the shearstress (entrance pressure) may be controlled, and the apparentshear rate measured.3.1.1.2 Mathematically, the apparent shear rate for a New-tonian fluid at the wall is gi
12、ven as follows:g532 QpD3(1)where:g = apparent shear rate,Q = quantity of fluid extruded in one second, mm3,p = the constant pi, approximately 3.142, andD = diameter of the measuring capillary, mm.The units of apparent shear rate are reciprocal seconds (s1).3.1.2 apparent shear stress (t)the measured
13、 resistance toflow through a capillary die; it may be determined by measur-ing the die entrance pressure for a specified die, then applyingappropriate geometric factors.1These test methods are under the jurisdiction of ASTM Committee D11 onRubber and are the direct responsibility of Subcommittee D11
14、.12 on ProcessabilityTests.Current edition approved Nov. 1, 2003. Published December 2003. Originallyapproved in 1993. Last previous edition approved in 1998 as D 5099 93 (1998).2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org.
15、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, United States.3.1.2.1 Mathematically, apparent shear stress is given asfollows:t5P
16、4L/D!(2)where:t = apparent shear stress,P = pressure at the entrance to the measuring capillary, Pa,L = length of the measuring capillary, mm, andD = diameter of the measuring capillary, mm.3.1.3 apparent viscosityratio of apparent shear stress toapparent shear rate.3.1.3.1 DiscussionFor an extrusio
17、n capillary rheometer,the ratio is usually calculated at a given shear rate. It isnormally expressed in Pascal seconds (Pa.s). 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
18、the measurement wasmade.3.1.4 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.3.1.5 corrected shear rate (gw)a shear rate at the w
19、all ofthe capillary die determined by applying the Rabinowitschcorrection for non-Newtonian materials.3.1.5.1 DiscussionThe Rabinowitsch correction math-ematically adjusts the shear rate values for the fact that the fluidis non-Newtonian, using the power law fluid model. To obtainthe corrected shear
20、 rate, at least two measurements of apparentshear stress and apparent shear rate are made, generally byincreasing the rate of extrusion (Q) with the same measuringcapillary. The Bagley correction of 3.1.6.2 is made to the shearstress values; either by algebraic means if only two measure-ments are ma
21、de, or by a regression equation for a greaternumber of points, (Eq 6) is solved for N8, using the correctedshear stress (tw). Although in theory, N (of (Eq 6) and N (of(Eq 3) should be identical, their respective values may vary asthe Bagley correction (E) varies, hence the designation of N8 in(Eq 3
22、).3.1.5.2 The corrected shear rate (gw) is therefore:gw5gF3N8 1 14NG(3)For most rubbers or elastomers the correction factor forshear rate is typically between 1.5 and 2.1, but there areexceptions.3.1.6 corrected shear stress (tw)the apparent shear stressat the wall of the capillary die; it is correc
23、ted by applying theBagley correction (E) (see 3.1.6.2) for energy losses at theentrance and exit of the die.3.1.6.1 Discussion 1Units are Pascals (Pa); however, thiscorrection is often applied as though it were an additionallength of capillary. The correction is often termed 88end effect.”Capillary
24、entrance angle and geometry have great influence onthe magnitude of this correction.3.1.6.2 Discussion 2Since the magnitude of correction isa function of shear rate, data for this correction are obtained byusing two or more dies of different lengths but of the samediameter (and thus same apparent sh
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