ASTM E2584-2010 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance (Slug) Calorimeter《使用热容(芯棒)热量计测定材料导热性的标准实施规程》.pdf
《ASTM E2584-2010 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance (Slug) Calorimeter《使用热容(芯棒)热量计测定材料导热性的标准实施规程》.pdf》由会员分享,可在线阅读,更多相关《ASTM E2584-2010 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance (Slug) Calorimeter《使用热容(芯棒)热量计测定材料导热性的标准实施规程》.pdf(11页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E2584 10Standard Practice forThermal Conductivity of Materials Using a ThermalCapacitance (Slug) Calorimeter1This standard is issued under the fixed designation E2584; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision, th
2、e 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 practice describes a technique for the determinationof the apparent thermal conductivity, la, of materi
3、als. It is forsolid materials with apparent thermal conductivities in theapproximate range 0.02 la 2 W/(mK) over the approxi-mate temperature range between 300 K and 1100 K.NOTE 1While the practice should also be applicable to determiningthe thermal conductivity of non-reactive materials, it has bee
4、n foundspecifically useful in testing fire resistive materials that are both reactiveand undergo significant dimensional changes during a high temperatureexposure.1.2 The values stated in SI units are to be regarded asstandard. No other units of measurement are included in thisstandard.1.3 This stan
5、dard 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 limitations prior to use.2. Referenced Documents2.1 A
6、STM Standards:2C1113 Test Method for Thermal Conductivity of Refracto-ries by Hot Wire (Platinum Resistance Thermometer Tech-nique)D2214 Test Method for Estimating the Thermal Conductiv-ity of Leather with the Cenco-Fitch Apparatus3E177 Practice for Use of the Terms Precision and Bias inASTM Test Me
7、thodsE220 Test Method for Calibration of Thermocouples ByComparison TechniquesE230 Specification and Temperature-Electromotive Force(EMF) Tables for Standardized ThermocouplesE457 Test Method for Measuring Heat-Transfer Rate Usinga Thermal Capacitance (Slug) CalorimeterE691 Practice for Conducting a
8、n Interlaboratory Study toDetermine the Precision of a Test Method3. Terminology3.1 Definitions:3.1.1 thermal conductivity, lthe time rate of heat flow,under steady conditions, through unit area, per unit temperaturegradient in the direction perpendicular to the area.3.1.2 apparent thermal conductiv
9、ity, lawhen other modesof heat transfer (and mass transfer) through a material arepresent in addition to thermal conduction, the results of themeasurements performed according to this practice will repre-sent the apparent or effective thermal conductivity for thematerial tested.3.2 Symbols:A = speci
10、men area normal to heat flux direction, m2Cp= specific heat capacity, J/(kgK)F = heating or cooling rate, (K/s)L = thickness of a specimen (slab) in heat transfer direc-tion, mM = mass, kgQ = heat flow, WT = absolute temperature, KTinnerSSS= mean temperature of the stainless steel slug, KTouterSPEC=
11、 mean temperature of outer (exposed) specimensurfaces, KTmeanSPEC= mean temperature of specimen, KDT = temperature difference across the specimen, given by(TouterSPEC TinnerSSS), Kl = thermal conductivity, W/(mK)la= apparent thermal conductivity, W/(mK)rSPEC= bulk density of specimen being tested, k
12、g/m33.3 Subscripts/Superscripts:SPEC = material specimen being evaluatedSSS = stainless steel slug (thermal capacitance transducer)1This practice is under the jurisdiction of ASTM Committee E37 on ThermalMeasurements and is the direct responsibility of Subcommittee E37.05 on Thermo-physical Properti
13、es.Current edition approved March 1, 2010. Published May 2010. Originallyapproved in 2007. Last previous edition approved in 2007 as E2584 07. DOI:10.1520/E2584-10.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Boo
14、k of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.3Withdrawn. The last approved version of this historical standard is referencedon www.astm.org.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, U
15、nited States.4. Summary of Practice4.1 Principle of OperationIn principle, a slug of ther-mally conductive metal, capable of withstanding elevatedtemperatures, is surrounded with another material of a uniformthickness (the specimen) whose thermal conductivity is sub-stantially lower than that of the
16、 slug. When the outer surface ofthis assembly is exposed to a temperature above that of theslug, heat will pass through the outer layer, causing a tempera-ture rise in the slug itself. The temperature rise of the slug iscontrolled by the amount and rate of heat conducted to itssurface (flux), its ma
17、ss, and its specific heat capacity. With theknowledge of these properties, the rate of temperature rise ofthe slug is in direct proportion to the heat flux entering it. Thus,under these conditions, the slug becomes a flux-gaugingdevice. From this measured flux, along with the measuredthermal gradien
18、t across the outer (specimen) layer, the apparentthermal conductivity of the specimen can be calculated. Whenthe heat source is removed, during natural cooling, the direc-tion of the heat flow will be reversed. Still, from the measuredflux and thermal gradient, the apparent thermal conductivitycan b
19、e calculated.4.2 Boundary ConditionsThe ideal model describedabove is based on heat flow toward the slug, perpendicularly tothe specimen, and always through the specimen. Deviatingfrom ideality can be due to:4.2.1 Thickness non-uniformity of the outer layer.4.2.2 Inhomogeneity (chemical or microstru
20、ctural) of theouter layer.4.2.3 Parasitic paths through cracks, gaps or other mechani-cally induced paths.4.2.4 Parasitic paths through wires, sheaths (thermo-couples), etc., that are unavoidable parts of a practical embodi-ment.4.2.5 Delamination of the specimen from the slugs surface(gap formation
21、).NOTE 2The user of this method should be very aware of the fact thatthe contact resistance between the specimen(s) and the slug may notalways be neglected, and in some cases may be even significant, becomingprobably the most important source of uncertainty in the measurement.For low-density porous
22、materials, however, it was found that, generally,the contact resistance between the specimen(s) and the slug may beneglected.4.3 ConfigurationsThis method lends itself to many pos-sible geometrical configurations, a few of which are listedbelow:4.3.1 For pipe (tubular) insulations, a cylindrical slu
23、g is tobe used. End faces are to be blocked with insulation.4.3.2 For flat plate stock (insulating boards, bulk materials,etc.), a rectangular shaped slug is considered most practical,with the specimen material covering:4.3.2.1 Both large faces of the slab, with the edges heavilyinsulated.4.3.2.2 On
24、e large face of the slab, with the other face andthe edges heavily insulated.4.4 OperationFor simplicity, only the rectangular em-bodiment is described below:4.4.1 Twin Specimens (Double-Sided)A sandwich testspecimen is prepared consisting of twin specimens of thematerial, of known mass and known an
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