ASTM E1980-2001 Standard Practice for Calculating Solar Reflectance Index of Horizontal and Low-Sloped Opaque Surfaces 《计算水平和低斜不透明表面阳光反射指数的标准实施规程》.pdf

《ASTM E1980-2001 Standard Practice for Calculating Solar Reflectance Index of Horizontal and Low-Sloped Opaque Surfaces 《计算水平和低斜不透明表面阳光反射指数的标准实施规程》.pdf》由会员分享，可在线阅读，更多相关《ASTM E1980-2001 Standard Practice for Calculating Solar Reflectance Index of Horizontal and Low-Sloped Opaque Surfaces 《计算水平和低斜不透明表面阳光反射指数的标准实施规程》.pdf（3页珍藏版）》请在麦多课文档分享上搜索。

1、Designation: E 1980 01Standard Practice forCalculating Solar Reflectance Index of Horizontal and Low-Sloped Opaque Surfaces1This standard is issued under the fixed designation E 1980; 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.INTRODUCTIONThe steady-state surface temperature (Ts) under the sun is strongly correlated to solar reflectivityand

3、thermal emissivity of the surface. For equivalent conditions, the Tsof dark surfaces (with low solarreflectance) is higher than light-colored surfaces (with high solar reflectance); and surfaces with lowthermal emissivity have higher Tss than surfaces with high thermal emissivity. The procedurerecom

4、mended in this standard will allow a direct comparison of Tsof surfaces under the sun. Theprocedure defines a Solar Reflectance Index (SRI) that measures the relative Tsof a surface withrespect to the standard white (SRI = 100) and standard black (SRI =0) under the standard solar andambient conditio

5、ns.1. Scope1.1 This practice covers the calculation of the Solar Reflec-tance Index (SRI) of horizontal and low-sloped opaque sur-faces at standard conditions. The method is intended tocalculate SRI for surfaces with emissivity greater than 0.1.1.2 This standard does not purport to address all of th

6、esafety 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 ASTM Standards:2E 408 Test Methods for Tota

7、l Normal Emittance of SurfacesUsing Inspection-Meter TechniquesE 772 Terminology Relating to Solar Energy ConversionE 891 Tables for Terrestrial Direct Normal Solar Irradiancefor Air Mass 1.53E 903 Test Method for Solar Absorption, Reflectance, andTransmittance of Materials Using Integrating Spheres

8、E 1918 Test Method for Measuring Solar Reflectance ofHorizontal and Low-Sloped Surfaces in the Field3. Terminology3.1 Definitions:3.1.1 convective coeffcient (hc)the rate of heat transferfrom the surface to air induced by the air movement, expressedin watts per square metre per degree Kelvin, Wm2K1.

9、3.1.2 low-sloped surfacessurfaces with a slope smallerthan 9.5 from the horizontal.3.1.3 reference black surface temperature (Tb)is thesteady-state temperature of a black surface with solar reflec-tance of 0.05 and thermal emissivity of 0.9, under the standardsolar and ambient conditions.3.1.4 refer

10、ence white surface temperature (Tw)is thesteady-state temperature of a white surface with solar reflec-tance of 0.80 and thermal emissivity of 0.9, under the standardsolar and ambient conditions.3.1.5 sky temperature (Tsky)is the temperature of a blackbody that would radiate the same power toward th

11、e earth asdoes the sky.3.1.6 solar absorptance (a)the fraction of solar fluxabsorbed by a surface. For an opaque surface a =1a.3.1.7 solar flux (I)is the direct and diffuse radiant powerfrom the sun received at ground level over the solar spectrum,expressed in watts per square metre, Wm2.3.1.8 solar

12、 reflectance (a)the fraction of solar flux re-flected by a surface.3.1.9 solar reflectance index (SRI)is the relative Tsof asurface with respect to the standard white (SRI = 100) andstandard black (SRI = 0) under the standard solar and ambientconditions.1This test method is under the jurisdiction of

13、ASTM Committee D08 on Roofingand Waterproofing and is the direct responsibility of Subcommittee D08.18 onNonbituminous Organic Roof Coverings.Current edition approved April 10, 2001. Published April 2001. Originallypublished as E 198098. Last previous edition E 198098e1.2For referenced ASTM standard

14、s, 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.3Withdrawn.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshoh

15、ocken, PA 19428-2959, United States.3.1.10 solar spectrumspectral distribution of typical ter-restrial sunlight at air mass 1.5 as defined in Tables E 891.3.1.11 standard solar and ambient conditions for thepurpose of this calculation, is defined as a solar flux of 1000Wm2, ambient air temperature o

16、f 310 Kelvin (K), and skytemperature of 300 K. Three convective coefficient of 5, 12, 30Wm2K1, corresponding to low- (0 to 2 ms1), medium- (2 to6ms1), and high-wind (6 to 10 ms1) conditions, respectively.3.1.12 steady-state surface temperature (Ts)is the tem-perature of the surface, in K, under the

17、standard solar andambient conditions.3.1.13 thermal emissivity (e)the ratio of radiant fluxemitted by a surface at a given temperature to that emitted bya black body radiator at the same temperature. For thiscalculation, the thermal emissivity is for a temperature below150C.4. Summary of Practice4.1

18、 For a surface exposed to the sun, when the conductioninto the material is zero, the steady-state surface temperature isobtained by:aI 5esTs4 Tsky4! 1 hcTs Ta! (1)where:a = solar absorptance=1solar reflectance,I = solar flux, Wm2,e = thermal emissivity,s = Stefan Boltzmann constant, 5.66961 x 108Wm2

19、K4,Ts= steady-state surface temperature, K,Tsky= sky temperature, K,hc= convective coefficient, Wm2K1, andTa= air temperature, K.4.2 Given the solar reflectivity and thermal emissivity of asurface, and the convective coefficient, Eq 1 needs to be solvediteratively for surface temperature. Alternativ

20、ely, one can usethe following equation to obtain the surface temperature:Ts5 309.07 11066.07a 31.98e!6.78e1hc!(2)890.94a21 2153.86ae!6.78e1hc!2Surface temperature estimated by Eq 2 is accurate within 1K.4.3 In this practice, Solar Reflectance Index is defined as:SRI 5 100Tb TsTb Tw(3)where: Tband Tw

21、are the steady-state temperature of blackand white surfaces.Under the standard solar and ambient conditions, Eq 3 isregressed to:SRI 5 123.97 141.35x19.655x2(4)where:x5a 0.029e!8.797 1 hc!9.5205e1hc(5)For a greater than 0.1, and excluding collector surfaces(surface with high solar absorptance and lo

22、w thermal emit-tance, that is, a greater than 0.8 and e less than 0.2), Eq 4estimates SRI with an average error of 0.9 and maximum errorof 2.5. Significance and Use5.1 Solar reflectance and thermal emittance are importantfactors affecting surface and near-surface ambient air tempera-ture. Surfaces w

23、ith low solar reflectance, absorb a high fractionof the incoming solar energy.Afraction of this absorbed energyis conducted into ground and buildings, a fraction is convectedto air (leading to higher air temperatures), and a fraction isradiated to the sky. For equivalent conditions, the lower theemi

24、ssivity of a surface the higher its steady-state temperature.Surfaces with low emissivity cannot effectively radiate to thesky and, therefore, get hot. Determination of solar reflectanceand thermal emittance, and subsequent calculation of therelative temperature of the surfaces with respect to black

25、 andwhite reference temperature (defined as Solar ReflectanceIndex, SRI), may help designers and consumers to choose theproper materials to make their buildings and communitiesenergy efficient. The method described here gives the SRI ofsurfaces based on measured solar reflectances and thermalemissiv

26、ities of the surfaces.6. Procedure6.1 Given the solar reflectance and thermal emissivity of atest surface, calculate the SRI for three convective coefficientsof 5, 12, 30 Wm2K1, corresponding to low-, medium-, andhigh-wind conditions, respectively. The following alternateapproaches can be used to ca

27、lculate SRI:6.1.1 Approach ICalculate the steady-state surface tem-peratures for the test surface and black and white referencesurfaces. Either Eq 1 (with iterative approach) or Eq 2 can beused. Calculate the SRI from Eq 3.6.1.2 Approach II Calculate SRI from Eq 4.7. Report7.1 The report shall inclu

28、de the following:7.1.1 The solar reflectance and the thermal emittance of thetest surface.7.1.2 The calculated SRI for three convective coefficients of5, 12, 30 Wm2K1, corresponding to low-, medium-, andhigh-wind conditions, respectively.8. Precision and Bias8.1 The SRI of a test surface varies with

29、 two materialproperties, solar reflectance and thermal emissivity, and fourenvironmental conditions, solar flux, convection coefficient, airtemperature, and sky temperature. A detailed sensitivity analy-sis for the variation of SRI with respect to the above environ-mental conditions has been reporte

30、d.4The following is asummary of the results and may be used as a guideline forpractitioners.4Akbari, H., R. Levinson, and P. Berdahl, “ASTM Standards for MeasuringSolar Reflectance and Infrared Emittance of Construction Materials and Comparingtheir Steady-State Surface Temperatures,” Proceedings of

31、the ACEEE 1996 SummerStudy on Energy Effciency in Buildings, Vol. 1, p. 1, Pacific Grove, CA, August1996.E19800128.1.1 SRI is an excellent predictor of solar reflectance formaterials with high emissivity (e 0.8), that is, non-metals.Under these conditions, a 61 % error in solar reflectance willresul

32、t in a maximum error of 61.4 in SRI. Similarly, a 61%error in e will result in a maximum error of 60.6 in SRI.8.1.2 For non-metallic surfaces, SRI is insensitive to choiceof convective coefficient.8.1.3 For metallic surfaces that are characterized with low e,the SRI calculated by the above procedure

33、 varies significantlywith the choice of convection coefficient. Hence, the SRIshould be reported for three convective coefficients corre-sponding to low-, medium-, and high-wind conditions.8.1.4 SRI is insensitive to choice of sky temperature,ambient temperature, and solar flux.9. Keywords9.1 solar

34、flux; solar reflectance; solar reflectance index;thermal emittanceASTM International takes no position respecting the validity of any patent rights asserted in connection with any item mentionedin this standard. Users of this standard are expressly advised that determination of the validity of any s

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37、a fair hearing you shouldmake your views known to the ASTM Committee on Standards, at the address shown below.This standard is copyrighted by ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959,United States. Individual reprints (single or multiple copies) of this standard may be obtained by contacting ASTM at the aboveaddress or at 610-832-9585 (phone), 610-832-9555 (fax), or serviceastm.org (e-mail); or through the ASTM website(www.astm.org).E1980013