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 qz between two gas layers is proportional to the energy density :qz µ c VnT
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 des liquides et des gaz. - Izdatelstvo Standartov,...
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