ASTM E2070-2008 Standard Test Method for Kinetic Parameters by Differential Scanning Calorimetry Using Isothermal Methods《用等温法的差示扫描量热法测定动力系数的标准试验》.pdf
《ASTM E2070-2008 Standard Test Method for Kinetic Parameters by Differential Scanning Calorimetry Using Isothermal Methods《用等温法的差示扫描量热法测定动力系数的标准试验》.pdf》由会员分享,可在线阅读,更多相关《ASTM E2070-2008 Standard Test Method for Kinetic Parameters by Differential Scanning Calorimetry Using Isothermal Methods《用等温法的差示扫描量热法测定动力系数的标准试验》.pdf(11页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E 2070 08Standard Test Method forKinetic Parameters by Differential Scanning CalorimetryUsing Isothermal Methods1This standard is issued under the fixed designation E 2070; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revisio
2、n, 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 Test Method A determines kinetic parameters for acti-vation energy, pre-exponential factor and reactio
3、n order usingdifferential scanning calorimetry from a series of isothermalexperiments over a small (; 10 K) temperature range. Thistreatment is applicable to low nth order reactions and toautocatalyzed reactions such as thermoset curing or pyrotech-nic reactions and crystallization transformations i
4、n the tem-perature range from 300 to 900 K (30 to 630 C). This testmethod is applicable only to these types of exothermic reac-tions when the thermal curves do not exhibit shoulders,discontinuities or shifts in baseline.1.2 Test Method B also determines the activation energy ofa set of time-to-event
5、 and isothermal temperature data gener-ated by this or other procedures.1.3 Test Method C determines the activation energy andinitial heat flow from a series of isothermal experiments over asmall temperature range. Because this approach only deter-mines kinetic parameter of activation energy, no kno
6、wledge ofthe kinetic model is required. Therefore it is considered to be“model free”. This approach is broadly applicable to a varietyof complicated reactions including those not well understood.1.4 SI units are the standard.1.5 This test method is similar but not equivalent to ISO11357, Part 5, and
7、 provides more information than the ISOstandard.1.6 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-priate safety and health practices and determine the applica-bility of reg
8、ulatory limitations prior to use. Specific precau-tionary statements are given in Section 8.2. Referenced Documents2.1 ASTM Standards:2D 3550 Practice for Thick Wall, Ring-Lined, Split Barrel,Drive Sampling of SoilsD 3895 Test Method for Oxidative-Induction Time of Poly-olefins by Differential Scann
9、ing CalorimetryD 4565 Test Methods for Physical and Environmental Per-formance Properties of Insulations and Jackets for Tele-communications Wire and CableD 5483 Test Method for Oxidation Induction Time of Lu-bricating Greases by Pressure Differential Scanning Calo-rimetryD 6186 Test Method for Oxid
10、ation Induction Time of Lu-bricating Oils by Pressure Differential Scanning Calorim-etry (PDSC)E 473 Terminology Relating to Thermal Analysis and Rhe-ologyE 537 Test Method for The Thermal Stability Of ChemicalsBy Differential Scanning CalorimetryE 698 Test Method for Arrhenius Kinetic Constants for
11、Thermally Unstable Materials Using Differential ScanningCalorimetry and the Flynn/Wall/Ozawa MethodE 967 Test Method for Temperature Calibration of Differ-ential Scanning Calorimeters and Differential ThermalAnalyzersE 968 Practice for Heat Flow Calibration of DifferentialScanning CalorimetersE 1142
12、 Terminology Relating to Thermophysical PropertiesE 1445 Terminology Relating to Hazard Potential ofChemicalsE 1860 Test Method for Elapsed Time Calibration of Ther-mal AnalyzersE 1958 Guide for Sensory Claim SubstantiationE 1970 Practice for Statistical Treatment of Thermoanalyti-cal Data1This test
13、 method is under the jurisdiction ofASTM Committee E37 on ThermalMeasurements and is the direct responsibility of Subcommittee E37.01 on ThermalTest Methods and Practices.Current edition approved Feb. 1, 2008. Published March 2008. Originallyapproved in 2000. Last previous edition approved in 2003 a
14、s E 2070 03.2For 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.1Copyright ASTM International, 100 Barr Harbor Dr
15、ive, PO Box C700, West Conshohocken, PA 19428-2959, United States.E 2041 Method for Estimating Kinetic Parameters by Dif-ferential Scanning Calorimeter Using the Borchardt andDaniels MethodE 2046 Test Method for Reaction Induction Time by Ther-mal Analysis2.2 ISO Standard:ISO DIS 11357 Part 5 Determ
16、ination of Temperature and/orTime of Reaction and Reaction Kinetics33. Terminology3.1 Specific technical terms used in this test method aredefined in Terminologies E 473, E 1142, and E 1445.4. Summary of Test Method4.1 A test specimen is held at a constant temperature in adifferential scanning calor
17、imeter throughout an exothermicreaction. The rate of heat evolution, developed by the reaction,is proportional to the rate of reaction. Integration of the heatflow as a function of time yields the total heat of reaction.4.2 An autocatalytic, nthorder data or model free treat-ment4,5,6is used to deri
18、ve the kinetic parameters of activationenergy, pre-exponential factor and reaction order from the heatflow and total heat of reaction information obtained in 4.1 (SeeBasis for Methodology, Section 5.)5. Basis of Methodology5.1 Reactions of practical consideration are exothermic innature; that is, th
19、ey give off heat as the reaction progresses.Furthermore, the rate of heat evolution is proportional to therate of the reaction. Differential scanning calorimetry measuresheat flow as a dependent experimental parameter. DSC isuseful for the measurement of the total heat of a reaction andthe rate of t
20、he reaction as a function of time and temperature.5.2 Reactions may be modeled with a number of suitableequations of the form of:da/dt 5 kT! fa! (1)where:da/dt = reaction rate (min1),a = fraction reacted or conversion (dimensionless),k (T) = specific rate constant at temperature T (min1),f(a) = conv
21、ersion function. Commonly used functionsinclude:f1a! 5 1a!n(2)f2a! 5am1a!n(3)where:n and m = partial reaction order terms.NOTE 1There are a large number of conversion function expressionsfor f(a)4. Those described here are the more common but are not theonly functions suitable for this method. Eq 2
22、is known as the general rateequation while Eq 3 is the autocatalytic (or Sestak-Berggren) equation5,6.Eq 2 is used for nth order reactions while Eq 3 is used for thermoset cureand crystallization transformations.5.3 For a reaction conducted at temperature (T), the auto-catalytic rate equation of 5.2
23、 may be cast in its logarithmicform.da/dt 5 kT! am1a!n(4)lnda/dt 5 lnkT!# 1 mlna 1 nln1 a (5)This equation has the form z = a + bx + cy and may be solvedusing multiple linear regression analysis.NOTE 2Subsequent discussions use the autocatalytic form of the rateequation (Eq 3). It reduces to the sim
24、pler general rate equation (Eq 2)when the value of reaction order parameter m equals zero thereby reducingthe number of kinetic parameters to be determined.5.4 The Arrhenius equation describes how the reaction ratechanges as a function of temperature:kT! 5 Ze2E/RT(6)where:Z = pre-exponential factor
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