ASTM E2584-2014 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance &40 Slug&41 Calorimeter《使用热电容40 弹头41 热量计测定材料导热性的标准实施规程》.pdf
《ASTM E2584-2014 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance &40 Slug&41 Calorimeter《使用热电容40 弹头41 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 E2584-2014 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance &40 Slug&41 Calorimeter《使用热电容40 弹头41 热量计测定材料导热性的标准实施规程》.pdf(12页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E2584 14Standard 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, a, of materia
3、ls. It is forsolid materials with apparent thermal conductivities in theapproximate range 0.02 a 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 been
4、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 standa
5、rd 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 AST
6、M Standards:2C1113 Test Method for Thermal Conductivity of Refracto-ries by Hot Wire (Platinum Resistance ThermometerTechnique)D2214 Test Method for Estimating the Thermal Conductiv-ity of Leather with the Cenco-FitchApparatus (Withdrawn2008)3E177 Practice for Use of the Terms Precision and Bias inA
7、STM Test MethodsE220 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 C
8、onducting an Interlaboratory Study toDetermine the Precision of a Test Method3. Terminology3.1 Definitions:3.1.1 thermal conductivity, the 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
9、 conductivity, awhen 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:
10、A = specimen 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, KTo
11、uterSPEC= mean temperature of outer (exposed) specimensurfaces, KTmeanSPEC= mean temperature of specimen, KT = temperature difference across the specimen, given by(TouterSPEC TinnerSSS), K = thermal conductivity, W/(mK)a= apparent thermal conductivity, W/(mK)SPEC= bulk density of specimen being test
12、ed, kg/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 Pro
13、perties.Current edition approved Feb. 15, 2014. Published March 2014. Originallyapproved in 2007. Last previous edition approved in 2010 as E2584 10. DOI:10.1520/E2584-14.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Ann
14、ual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.3The last approved version of this historical standard is referenced onwww.astm.org.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United
15、 States14. Summary of Practice4.1 Principle of OperationIn principle, a slug of thermallyconductive 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 slug.
16、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 mass, and
17、 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 gradient acros
18、s 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 be calcu
19、lated.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 microstructural)
20、 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(thermocouples), etc., that are unavoidable parts of a practicalembodiment.4.2.5 Delamination of the specimen from the slugs surface(gap formation).NOTE 2The
21、 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 materials,
22、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 slug is tobe u
23、sed. 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 One large fac
24、e 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 and nominally
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