ASTM E2584-2007 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance (Slug) Calorimeter《用热电容(散热片)量热计测定材料导热性的标准实施规程》.pdf
《ASTM E2584-2007 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance (Slug) Calorimeter《用热电容(散热片)量热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 E2584-2007 Standard Practice for Thermal Conductivity of Materials Using a Thermal Capacitance (Slug) Calorimeter《用热电容(散热片)量热计测定材料导热性的标准实施规程》.pdf(9页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: E 2584 07Standard Practice forThermal Conductivity of Materials Using a ThermalCapacitance (Slug) Calorimeter1This standard is issued under the fixed designation E 2584; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision,
2、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 This practice describes a technique for the determinationof the apparent thermal conductivity, la, of mat
3、erials. 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
4、been foundspecifically useful in testing fire resistive materials that are both reactiveand undergo significant dimensional changes during a high temperatureexposure.1.2 This standard does not purport to address all of thesafety concerns, if any, associated with its use. It is theresponsibility of t
5、he 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:2C 1113 Test Method for Thermal Conductivity of Refracto-ries by Hot Wire (Platinum Resistance Thermometer
6、Tech-nique)D 2214 Test Method for Estimating the Thermal Conduc-tivity of Leather with the Cenco-Fitch ApparatusE 220 Test Method for Calibration of Thermocouples ByComparison TechniquesE 230 Specification and Temperature-Electromotive Force(EMF) Tables for Standardized ThermocouplesE 457 Test Metho
7、d for Measuring Heat-Transfer Rate Usinga Thermal Capacitance (Slug) CalorimeterE 691 Practice for Conducting an 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
8、 area, per unit temperaturegradient in the direction perpendicular to the area.3.1.2 apparent thermal conductivity, 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 pract
9、ice will repre-sent the apparent or effective thermal conductivity for thematerial tested.3.2 Symbols: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
10、 = heat flow, WT = absolute temperature, KTinnerSSS= mean temperature of the stainless steel slug, KTouterSPEC= mean temperature of outer (exposed) specimensurfaces, KTmeanSPEC= mean temperature of specimen, KDT = temperature difference across the specimen, given by(TouterSPEC TinnerSSS), K,l = ther
11、mal conductivity, W/(mK)la= apparent thermal conductivity, W/(mK)rSPEC= bulk density of specimen being tested, kg/m33.3 Subscripts/Superscripts:SPEC = material specimen being evaluatedSSS = stainless steel slug (thermal capacitance transducer)4. Summary of Practice4.1 Principle of OperationIn princi
12、ple, 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 slug. When the outer surface ofthis assembly is exposed to a temperat
13、ure 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 its specific heat capacity. With theknowledge of these propert
14、ies, the rate of temperature rise of1This practice is under the jurisdiction of ASTM Committee E37 on ThermalMeasurements and is the direct responsibility of Subcommittee E37.05 on Thermo-physical Properties.Current edition approved Sept. 1, 2007. Published November 2007.2For referenced ASTM standar
15、ds, 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 Drive, PO Box C700, West Conshohocken, PA
16、19428-2959, United States.Copyright by ASTM Intl (all rights reserved); Fri Oct 31 01:42:58 EST 2008Downloaded/printed byGuo Dehua (CNIS) pursuant to License Agreement. No further reproductions authorized.the slug is in direct proportion to the heat flux entering it. Thus,under these conditions, the
17、 slug becomes a flux-gaugingdevice. From this measured flux, along with the measuredthermal gradient 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
18、reversed. Still, from the measuredflux and thermal gradient, the apparent thermal conductivitycan be 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
19、due to:4.2.1 Thickness non-uniformity of the outer layer.4.2.2 Inhomogeneity (chemical or microstructural) 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
20、of a practical embodi-ment.4.2.5 Delamination of the specimen from the slugs surface(gap formation).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, be
21、comingprobably the most important source of uncertainty in the measurement.For low-density porous 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 conf
22、igurations, a few of which are listedbelow:4.3.1 For pipe (tubular) insulations, a cylindrical slug 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
23、material covering:4.3.2.1 Both large faces of the slab, with the edges heavilyinsulated.4.3.2.2 One 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 sandwic
24、h testspecimen is prepared consisting of twin specimens of thematerial, of known mass and known and nominally identicalthickness, between which is sandwiched a stainless steelthermal capacitance transducer (slug) of known mass. Theentire sandwich is placed between two (high temperature)metal retaini
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