The kinetic theory of gases assumes that all molecules are non-interacting rigid spheres of mass m and diameter σ moving at an average velocity v. The number of molecules per unit volume is n. Under the influence of a temperature gradient, the molecules move, collide and bring a certain amount of energy into play. This energy flow q
z
between two gas layers is proportional to the energy density :
q
z
µ c
V
nT
with :
c
V
:
constant-volume heat capacity per molecule
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(1) - VARGAFTIK (N. V.), FILIPPOV (L. P.), TARZIMANOV (A. A.), IORCHAK (R. P.) -
Conductivité thermique des gaz et des liquides.
-
Izdatelstvo Standartov, Moscou (1970).
(2) - VARGAFTIK (L. P.), FILIPPOV (L. P.), TARZIMANOV (A. A.), TOTSKIN (E. E.) -
Conductivité thermique...
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