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Heat current : ウィキペディア英語版
Heat current

A heat current is a kinetic exchange rate between molecules, relative to the material in which the kinesis occurs. It is defined as \frac, where Q is heat and t is time.
For conduction, heat current is defined by Fourier's law as
: \frac = -k \oint_S}
where
:\big. \frac\big. is the amount of heat transferred per unit time () and
:
:\overrightarrow is an oriented surface area element ()
The above differential equation, when integrated for a homogeneous material of 1-D geometry between two endpoints at constant temperature, gives the heat flow rate as:
: \big. \frac = -k A \frac
where
: ''A'' is the cross-sectional surface area,
: \Delta T is the temperature difference between the ends,
: \Delta x is the distance between the ends.
For thermal radiation, heat current is defined as
:W = \sigma \cdot A \cdot T^4
where the constant of proportionality \sigma is the Stefan–Boltzmann constant, A is the radiating surface area, and T is temperature.
Heat current can also be thought of as the total phonon distribution multiplied by the energy of one phonon, times the group velocity of the phonons. The phonon distribution of a particular phonon mode is given by the Bose-Einstein factor, which is dependent on temperature and phonon energy.
==See also==

* Thermal conduction
* Thermal conductivity

de:Wärmestrom
eo:Varmokurento

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Heat current」の詳細全文を読む



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