next up previous
Next: Thermal conduction Up: Heat Flow Previous: Heat Flow

Radiation

Matter at finite temperatures emits electromagnetic radiation with a wave length distribution which peaks approximately for
eqnarray29
Where tex2html_wrap_inline108 Js is Plancks constant. Putting in numbers we find for a hot bonfire where tex2html_wrap_inline110 K
eqnarray36
Such radiation is called thermal radiation. We cannot see it because its wave length is too long for our eyes and we cannot pick it up on our radio dial because the frequency is too high. The radiation is generally called infra red radiation because its wave length is longer than that corresponding to red light. The total radiation emitted per area unit is given by Stefan Boltzmans law
equation42
where tex2html_wrap_inline112 W/(mtex2html_wrap_inline114Ktex2html_wrap_inline116) and tex2html_wrap_inline118 is a thermal emissivity factor which is 1 for a perfectly absorbing so called black body and very small for a perfectly reflecting surface. Bodies are as efficient at absorbing thermal radiation as they are at emitting it. If it were not so then it would be impossible to establish thermal equilibrium through the thermal radiation phenomenon. Thus the net absorbed radiation from an environment at temperature tex2html_wrap_inline120 to a body at temperature tex2html_wrap_inline122 is
equation47
This explains why you feel cold on a cold night even when there is no wind: Your body is radiating more thermal energy to the surroundings than it is picking up in return. We have a demonstration experiment which illustrates the different thermal emissivities of various materials. We find that the more shiny the less emissivity. This is perhaps part of the reason why industrial grade refrigerators are made from polished stainless steel.



Collin Broholm
Tue Nov 25 23:12:10 EST 1997