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CHAPTER 9
1955' Gui
employed in building construction, the radiation and convection-conduc tion components may vary independently of each other.
Table 1, Section B, gives the thermal conductances and resistances of air spaces of uniform thickness and moderately smooth surfaces, based on experimental measurements conducted at the National Bureau of. Standi ards.* Although the conductances of air spaces vary to some extent with, thickness in the range over % in., average values are tabulated for thev, range from % in. to 4 in., for all except horizontal spaces with heat flow,V downward. The error involved by averaging is less than 10 percent in <
Fig. 4. Curves Showing Relation Between Surface Conductances foe .
Different Surfaces at 20 F Mean Temperature
the extreme case and less than 5 percent in most. For more exact values]:
Reference 9 may be consulted.
For narrow air spaces, which may be defined as those for which the;
product of the cube of the thickness of the space in inches times the terife,,.
perature difference (Fahrenheit degrees) across the space is less than'3?
for heat flow horizontally or downward, or less than 1 for heat flow up),]
ward, the conductance is the sum of the radiative heat transfer coefficient.
and that for conduction alone through air, since convection is practically;: suppressed. The radiation component can be computed by means ok
Equation 4 and Table 4 of Chapter 5; the conduction component can h?:
computed using the conductivity of air at the appropriate mean temperar
ture.
(S'
The effects of different mean temperatures, temperature differences, and)
effective emissivities are indicated in Table 1, Section B. As indicate]; use may be made of interpolation and moderate extrapolation of con?-, ductance values in the table to obtain conductances for conditions modery'
Heat Transmission Coefficients of Building Materials
177
ately different from those given. Interpolation of resistance values is not recommended, especially in relation to emissivity values.
Table 1, Section C gives values for the surface reflectivities and emis sivities of materials used as boundaries of air spaces in building construc tion, for total radiation at ordinary building temperatures. Effective emissivities for various combinations of these materials, for use in con junction with Section B of Table 1, are given in the last two columns of Section C.
When considering heat transfer across air spaces in building construction, the emissivities of the boundary surfaces should be known. The possi bility of change in emissivity of highly reflective surfaces due to exposure to conditions promoting chemical action, deposition of dust, or soiling of the surface, must be considered in selecting a material for use.10
PRACTICAL COEFFICIENTS AND THEIR USE
For practical purposes it is necessary to compute average. coefficients that may be applied to various materials and types of construction. Table 2, as revised in this issue, gives representative values for dry materials at 70 F mean temperature, as selected by the ASHAE Technical Advisory; Committee on Insulation. Since there may be some variation in .the materials and in test conditions, these selected values may not be in exact agreement with published data of all manufacturers. The exact .valubTor the conductivity or conductance of a certain manufacturer's material can only be secured from unbiased tests or guaranteed by the manufacturer.
Tables 5 and 7 through 19 have not been revised in this edition due to the extensive computations involved. These tables are now in the proc ess ' of revision, and until new values are available, the Values given in the tables may be used with the assurance that the U-values will not be in error by an amount greater than would be anticipated from normal variations in the materials to which they apply. Tables 7 through 19 illustrate typical examples of constructions frequently encountered. The U-values for constructions not given, or for conditions where more accurate values are desired, may be computed by the use of the conductivity and conductance values shown in Table 2 or obtained from the manufacturer.
Caution
The user should realize that the average conductivity and conductance values given in Tables 2 or 5 do not necessarily apply to all products of the samc general description. In using these values, judgment should be exer cised with regard to the extent to which the product (either as received or as applied) will comply with the tabulated values. Exact conductivities or conductances for specific materials should be obtained from the manu facturer.
Due to the inconsistency of actual building construction, because of the human element, many designers do not use overall coefficients of transmiss>on lower than 0.10 for walls and particularly roofs, except where the instruction is installed under continuous supervision. It should also be uoted that these coefficients do not include any factor of safety and that ^hen no supervision is used, some designers incorporate a 10 percent actor of safety.