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dc.contributor.authorLienhard V, John H.
dc.date.accessioned2019-09-18T09:04:27Z
dc.date.available2019-09-18T09:04:27Z
dc.date.copyright3/27/2019 12:00:00 AM
dc.date.issued2019
dc.identifier.issn0022-1481
dc.identifier.otherht_141_05_052701.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4258542
dc.description.abstractThe radiation fractional function is the fraction of black body radiation below a given value of λT. Edwards and others have distinguished between the traditional, or “external,” radiation fractional function and an “internal” radiation fractional function. The latter is used for linearization of net radiation from a nongray surface when the temperature of an effectively black environment is not far from the surface's temperature, without calculating a separate total absorptivity. This paper examines the analytical approximation involved in the internal fractional function, with results given in terms of the incomplete zeta function. A rigorous upper bound on the difference between the external and internal emissivity is obtained. Calculations using the internal emissivity are compared to exact calculations for several models and materials. A new approach to calculating the internal emissivity is developed, yielding vastly improved accuracy over a wide range of temperature differences. The internal fractional function should be used for evaluating radiation thermal resistances, in particular.
dc.publisherAmerican Society of Mechanical Engineers (ASME)
dc.titleLinearization of Nongray Radiation Exchange: The Internal Fractional Function Reconsidered
dc.typeJournal Paper
dc.journal.volume141
dc.journal.issue5
dc.journal.titleJournal of Heat Transfer
dc.identifier.doi10.1115/1.4042158
dc.journal.fristpage52701
dc.journal.lastpage052701-9
dc.treeJournal of Heat Transfer:;2019:;volume( 141 ):;issue: 005
dc.contenttypeFulltext


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