ASTM E457-2008(2015) 3814 Standard Test Method for Measuring Heat-Transfer Rate Using a Thermal Capacitance (Slug) Calorimeter《用热容量 (芯棒) 热量计测量传热速率的标准试验方法》.pdf
《ASTM E457-2008(2015) 3814 Standard Test Method for Measuring Heat-Transfer Rate Using a Thermal Capacitance (Slug) Calorimeter《用热容量 (芯棒) 热量计测量传热速率的标准试验方法》.pdf》由会员分享,可在线阅读,更多相关《ASTM E457-2008(2015) 3814 Standard Test Method for Measuring Heat-Transfer Rate Using a Thermal Capacitance (Slug) Calorimeter《用热容量 (芯棒) 热量计测量传热速率的标准试验方法》.pdf(6页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E457 08 (Reapproved 2015)Standard Test Method forMeasuring Heat-Transfer Rate Using a Thermal Capacitance(Slug) Calorimeter1This standard is issued under the fixed designation E457; the number immediately following the designation indicates the year oforiginal adoption or, in the case o
2、f 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 describes the measurement of heattransfer rate using a thermal capacitance-ty
3、pe calorimeterwhich assumes one-dimensional heat conduction into a cylin-drical piece of material (slug) with known physical properties.1.2 The values stated in SI units are to be regarded asstandard. No other units of measurement are included in thisstandard.NOTE 1For information see Test Methods E
4、285, E422, E458, E459,and E511.1.3 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 regulatory limitatio
5、ns prior to use.2. Referenced Documents2.1 ASTM Standards:2E285 Test Method for Oxyacetylene Ablation Testing ofThermal Insulation MaterialsE422 Test Method for Measuring Heat Flux Using a Water-Cooled CalorimeterE458 Test Method for Heat of AblationE459 Test Method for Measuring Heat Transfer Rate
6、Usinga Thin-Skin CalorimeterE511 Test Method for Measuring Heat Flux Using a Copper-Constantan Circular Foil, Heat-Flux Transducer3. Summary of Test Method3.1 The measurement of heat transfer rate to a slug orthermal capacitance type calorimeter may be determined fromthe following data:3.1.1 Density
7、 and specific heat of the slug material,3.1.2 Length or axial distance from the front face of thecylindrical slug to the back-face thermocouple,3.1.3 Slope of the temperaturetime curve generated bythe back-face thermocouple, and3.1.4 Calorimeter temperature history.3.2 The heat transfer rate is thus
8、 determined numerically bymultiplying the density, specific heat, and length of the slug bythe slope of the temperaturetime curve obtained by the dataacquisition system (see Eq 1).3.3 The technique for measuring heat transfer rate by thethermal capacitance method is illustrated schematically in Fig.
9、1. The apparatus shown is a typical slug calorimeter which, forexample, can be used to determine both stagnation region heattransfer rate and side-wall or afterbody heat transfer ratevalues. The annular insulator serves the purpose of minimizingheat transfer to or from the body of the calorimeter, t
10、husapproximating one-dimensional heat flow. The body of thecalorimeter is configured to establish flow and should have thesame size and shape as that used for ablation models or testspecimens.3.3.1 For the control volume specified in this test method, athermal energy balance during the period of ini
11、tial lineartemperature response where heat losses are assumed negligiblecan be stated as follows:Energy Received by the Calorimeter front face!5Energy Conducted Axially Into the Slugqc5 Cpl T/! 5 MCp/A!T/! (1)where:qc= calorimeter heat transfer rate, W/m2, = density of slug material, kg/m3,Cp= avera
12、ge specific heat of slug material during thetemperature rise (T), J/kgK,l = length or axial distance from front face of slug to thethermocouple location (back-face), m,T =(Tf Ti) = calorimeter slug temperature rise duringexposure to heat source (linear part of curve), K, =(f i) = time period corresp
13、onding to T tempera-ture rise, s,M = mass of the cylindrical slug, kg,A = cross-sectional area of slug, m2.1This test method is under the jurisdiction of ASTM Committee E21 on SpaceSimulation andApplications of Space Technology and is the direct responsibility ofSubcommittee E21.08 on Thermal Protec
14、tion.Current edition approved May 1, 2015. Published June 2015. Originallyapproved in 1972. Last previous edition approved in 2008 as E457 08. DOI:10.1520/E0457-08R15.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual
15、Book of ASTMStandards 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 States1In order to determine the steady-state heat transfer rate witha thermal capacita
16、nce-type calorimeter, Eq 1 must be solved byusing the known properties of the slug material3(for example,density and specific heat)the length of the slug, and the slope(linear portion) of the temperaturetime curve obtained duringthe exposure to a heat source. The initial and final temperaturetransie
17、nt effects must be eliminated by using the initial linearportion of the curve (see Fig. 2).3.3.2 In order to calculate the initial response time for agiven slug, Eq 2 may be used.4This equation is based on theidealization of zero heat losses from slug to its holder.R5l2Cpk2lnS21 2q indicatedq inputD
18、(2)where:k = thermal conductivity of slug material, W/mKqindicated= q that would be measured at the back-face of theslug by Eq 1, W/m2qinput= constant qinputat the front-face of the slug begin-ning at =0,W/m23.3.3 Although the goal of good slug calorimeter design isto minimize heat losses, there can
19、 be heating environments,such as very high heat fluxes, where even a good slugcalorimeter design cannot meet the recommended 5 % maxi-mum heat loss criterion of 6.1. Also, this criterion only dealswith heat losses measured during the cooling phase, not lossesduring the heating phase, which can be gr
20、eater than the coolinglosses. Under these circumstances, significant heat losses fromslug to holder during the heating phase, as well as otherpossible decaying processes such as a drop in surfacecatalycity, can cause the Temperature-Time slope to decreasesignificantly more than can be accounted for
21、by the increasingheat capacity with temperature of the Copper slug alone,making it important that the slope be taken early in the processbefore the losses lower the slope too much, introducing moreerror to the downside on the heat flux calculated (see Fig. 3).The degree of losses affect the exact po
22、sition where the bestslope begins to occur, but typically it should be expected atabout time = Rcalculated by Eq 2 for qindicated/qinput= 0.99,which value of Ris abbreviated as R0.99. Fig. 2 and Fig. 3assume that “heat source on” is a step function. This is anidealization, but the reality can be sig
23、nificantly different. Forexample, in some cases a calorimeter may experience a higherheat flux prior to reaching its final position in the heat source,which can cause the initial maximum slope to be higher thanwhat is wanted for the calculation of the heat flux at the finalposition. Therefore, it is
24、 important to note that “zero” time, towhich R0.99is added to determine where to start looking forthe desired slope, is when the calorimeter has reached its finalposition where it is desired to measure the heat flux. Therefore,choosing the best place to take the slope can be very important.Should mo
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