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Balance of Entropy - The Onsager Reciprocal Relations

This case corresponds to a two-phase vapor-liquid state. From conditions F(0) 0 and F(l) 0 it follows that a necessary condition of biphasic state is [Pg.93]

This case corresponds to a one-phase saturated state (condensation point). From condition F(l) = 0 there follows the necessary condition of existence of mixture in a saturated gas state [Pg.93]

Note that criteria 1 and 5 are not physically realizable, therefore they may be considered only as the auxiliary criteria helpful in numerical solutions of appropriate problems. [Pg.93]

we have the following system of 2N + 2 equations for 2N + 2 unknowns [Pg.93]


See other pages where Balance of Entropy - The Onsager Reciprocal Relations is mentioned: [Pg.93]    [Pg.93]    [Pg.95]    [Pg.97]    [Pg.99]    [Pg.101]    [Pg.93]    [Pg.93]    [Pg.95]    [Pg.97]    [Pg.99]    [Pg.101]    [Pg.748]    [Pg.750]    [Pg.260]    [Pg.311]    [Pg.732]    [Pg.734]    [Pg.311]   


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Onsager

Onsager reciprocal relation

Onsager reciprocity relation

Onsager relation

Reciprocal relations

Reciprocity relation

The Entropy

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