Sol-air temperature: Difference between revisions

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|Display title=sol&ndash;air temperature
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|Meaning=The [[temperature]] that, under conditions of no [[direct solar radiation]] and no  air motion, would cause the same [[heat transfer]] into a house as that caused by the interplay of  all existing atmospheric conditions.
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|Explanation=It is given by the formula  <blockquote>[[File:ams2001glos-Se35.gif|link=|center|ams2001glos-Se35]]</blockquote> where &theta; is the sol&ndash;air temperature, ''T'' the outdoor [[air temperature]], ''a'' the radiational [[absorptivity]]  of the wall surface, ''I'' the incident [[radiation]], ''c'' the coefficient of convective heat transfer between  air and building material, and ''E'' the difference between the [[longwave radiation]] emitted and  received by the surface. In practice, this equation has been reduced to  <blockquote>[[File:ams2001glos-Se36.gif|link=|center|ams2001glos-Se36]]</blockquote> where &theta;, ''T'', and ''I'' are the <br/>''same as'' above; ''a''&prime; is a constant for construction material; and ''c''&prime; is a  constant for [[climate]].<br/> Landsberg, H. E. 1954. Bioclimatology of housing. Recent Studies in Bioclimatology, Meteor. Monogr.. 2(8).  p. 86.  
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== sol&ndash;air temperature ==
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<div class="definition"><div class="short_definition">The [[temperature]] that, under conditions of no [[direct solar radiation]] and no  air motion, would cause the same [[heat transfer]] into a house as that caused by the interplay of  all existing atmospheric conditions.</div><br/> <div class="paragraph">It is given by the formula  <div class="display-formula"><blockquote>[[File:ams2001glos-Se35.gif|link=|center|ams2001glos-Se35]]</blockquote></div> where &theta; is the sol&ndash;air temperature, ''T'' the outdoor [[air temperature]], ''a'' the radiational [[absorptivity]]  of the wall surface, ''I'' the incident [[radiation]], ''c'' the coefficient of convective heat transfer between  air and building material, and ''E'' the difference between the [[longwave radiation]] emitted and  received by the surface. In practice, this equation has been reduced to  <div class="display-formula"><blockquote>[[File:ams2001glos-Se36.gif|link=|center|ams2001glos-Se36]]</blockquote></div> where &theta;, ''T'', and ''I'' are the <br/>''same as'' above; ''a''&prime; is a constant for construction material; and ''c''&prime; is a  constant for [[climate]].</div><br/> </div><div class="reference">Landsberg, H. E. 1954. Bioclimatology of housing. Recent Studies in Bioclimatology, Meteor. Monogr.. 2(8).  p. 86. </div><br/>
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Latest revision as of 07:14, 30 March 2024

The temperature that, under conditions of no direct solar radiation and no air motion, would cause the same heat transfer into a house as that caused by the interplay of all existing atmospheric conditions.
It is given by the formula
ams2001glos-Se35
where θ is the sol–air temperature, T the outdoor air temperature, a the radiational absorptivity of the wall surface, I the incident radiation, c the coefficient of convective heat transfer between air and building material, and E the difference between the longwave radiation emitted and received by the surface. In practice, this equation has been reduced to
ams2001glos-Se36
where θ, T, and I are the
same as above; a′ is a constant for construction material; and c′ is a constant for climate.
Landsberg, H. E. 1954. Bioclimatology of housing. Recent Studies in Bioclimatology, Meteor. Monogr.. 2(8). p. 86.
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