ASTM C680-2004e4 Standard Practice for Estimate of the Heat Gain or Loss and the Surface Temperatures of Insulated Flat Cylindrical and Spherical Systems by Use of Computer Program.pdf
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1、Designation: C 680 04e4Standard Practice forEstimate of the Heat Gain or Loss and the SurfaceTemperatures of Insulated Flat, Cylindrical, and SphericalSystems by Use of Computer Programs1This standard is issued under the fixed designation C 680; the number immediately following the designation indic
2、ates the year oforiginal adoption or, in the case of revision, 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.e1NOTEFootnote 3 was editorially revised in November 2
3、004.e2NOTETable A1.1 was editorially corrected in August 2005.e3NOTEFootnote 3 and Section 2.3 were editorially deleted in September 2006.e4NOTE Table A1.1 was editorially corrected in June 2007.1. Scope1.1 This practice provides the algorithms and calculationmethodologies for predicting the heat lo
4、ss or gain and surfacetemperatures of certain thermal insulation systems that canattain one dimensional, steady- or quasi-steady-state heattransfer conditions in field operations.1.2 This practice is based on the assumption that the thermalinsulation systems can be well defined in rectangular, cylin
5、dri-cal or spherical coordinate systems and that the insulationsystems are composed of homogeneous, uniformly dimen-sioned materials that reduce heat flow between two differenttemperature conditions.1.3 Qualified personnel familiar with insulation-systemsdesign and analysis should resolve the applic
6、ability of themethodologies to real systems. The range and quality of thephysical and thermal property data of the materials comprisingthe thermal insulation system limit the calculation accuracy.Persons using this practice must have a knowledge of thepractical application of heat transfer theory re
7、lating to thermalinsulation materials and systems.1.4 The computer program that can be generated from thealgorithms and computational methodologies defined in thispractice is described in Section 7 of this practice.The computerprogram is intended for flat slab, pipe and hollow sphereinsulation syste
8、ms. An executable version of a program basedon this standard may be obtained from ASTM.1.5 The values stated in inch-pound units are to be regardedas the standard. The values given in parentheses are forinformation only.1.6 This standard does not purport to address all of thesafety concerns, if any,
9、 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 ASTM Standards:2C 168 Terminology Relating to Thermal Insulating Mat
10、eri-alsC 177 Test Method for Steady-State Heat Flux Measure-ments and Thermal Transmission Properties by Means ofthe Guarded Hot Plate ApparatusC 335 Test Method for Steady-State Heat Transfer Proper-ties of Horizontal Pipe InsulationC 518 Test Method for Steady-State Heat Flux Measure-ments and The
11、rmal Transmission Properties by Means ofthe Heat Flow Meter ApparatusC 585 Practice for Inner and Outer Diameters of RigidThermal Insulation for Nominal Sizes of Pipe and Tubing(NPS System)C 1055 Guide for Heated System Surface Conditions ThatProduce Contact Burn InjuriesC 1057 Practice for Determin
12、ation of Skin Contact Tem-perature from Heated Surfaces Using a MathematicalModel and Thermesthesiometer2.2 Other Document:NBS Circular 564 Tables of Thermodynamic and TransportProperties of Air, U.S. Dept of Commerce3. Terminology3.1 DefinitionsFor definitions of terms used in this prac-tice, refer
13、 to Terminology C 168.3.1.1 thermal insulation systemfor this practice, a thermalinsulation system is a system comprised of a single layer orlayers of homogeneous, uniformly dimensioned material(s)1This practice is under the jurisdiction of ASTM Committee C16 on ThermalInsulation and is the direct r
14、esponsibility of Subcommittee C16.30 on ThermalMeasurement.Current edition approved May 1, 2004. Published June 2004. Originallyapproved in 1971. Last previous edition approved in 2003 as C 680 - 03a.2For referenced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Servic
15、e 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 19428-2959, United States.intended for reduction of heat transfer betwee
16、n two differenttemperature conditions. Heat transfer in the system is steady-state. Heat flow for a flat system is normal to the flat surface,and heat flow for cylindrical and spherical systems is radial.3.2 SymbolsThe following symbols are used in the devel-opment of the equations for this practice
17、. Other symbols willbe introduced and defined in the detailed description of thedevelopment.where:h = surface transfer conductance, Btu/(hft2F) (W/(m2K) hiat inside surface; hoat outside surfacek = apparent thermal conductivity, Btuin./(hft2F) (W/(mK)ke= effective thermal conductivity over a prescri
18、bed tem-perature range, Btuin./(hft2F) (W/(mK)q = heat flux, Btu/(hft2) (W/m2)qp= time rate of heat flow per unit length of pipe,Btu/(hft) (W/m)R = thermal resistance, Fhft2/Btu (Km2/W)r = radius, in. (m); rm+1 rm= thicknesst = local temperature, F (K)ti= inner surface temperature of the insulation,
19、 F (K)t1= inner surface temperature of the systemto= temperature of ambient fluid and surroundings, F(K)x = distance, in. (m); xm+1 xm= thicknesse = effective surface emittance between outside surfaceand the ambient surroundings, dimensionlesss = Stefan-Boltzmann constant, 0.1714 3 10-8Btu/(hft2R4)
20、(5.6697 3 10-8W/(m2K4)Ts= absolute surface temperature, R (K)To= absolute surroundings (ambient air if assumed thesame) temperature, R (K)Tm=(Ts+ To)/2L = characteristic dimension for horizontal and verticalflat surfaces, and vertical cylindersD = characteristic dimension for horizontal cylinders an
21、dspherescp= specific heat of ambient fluid, Btu/(lbR) (J/(kgK)hc= average convection conductance, Btu/(hft2F) (W/(m2K)kf= thermal conductivity of ambient fluid, Btu/(hftF)(W/(mK)V = free stream velocity of ambient fluid, ft/h (m/s)y = kinematic viscosity of ambient fluid, ft2/h (m2/s)g = acceleratio
22、n due to gravity, ft/h2(m/s2)b = volumetric thermal expansion coefficient of ambientfluid, R-1(K-1)r = density of ambient fluid, lb/ft3(kg/m3)DT = absolute value of temperature difference betweensurface and ambient fluid, R (K)Nu = Nusselt number, dimensionlessRa = Rayleith number, dimensionlessRe =
23、 Reynolds number, dimensionlessPr = Prandtl number, dimensionless4. Summary of Practice4.1 The procedures used in this practice are based onstandard, steady-state, one dimensional, conduction heat trans-fer theory as outlined in textbooks and handbooks, Refs(4,5,20,21,22,30). Heat flux solutions are
24、 derived for tempera-ture dependent thermal conductivity in a material. Algorithmsand computational methodologies for predicting heat loss orgain of single or multi-layer thermal insulation systems areprovided by this practice for implementation in a computerprogram. In addition, interested parties
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