Relationships between the conductance and resistance phenomenological coefficients

Example 3.10 Relationships between the conductance and resistance phenomenological coefficients For a 

After applying the Onsager relations to the linear matrix solutions, we have 

Example 3.11 Transformation of phenomenological equations dependent flows Transform the thermodynamic forces and flows when the forces are independent, while the flows are linearly dependent in a two-flow system 0 y./t +J2. 

Using the linear relation between the flows, 0 =yJl + J2, Eq. (3.235) becomes 

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Example 3.10 Relationships between the conductance and resistance phenomenological coefficients For a three-flow system, to derive the relationships between the conductance and resistance phenomenological coefficients. Consider the linear phenomenological equations relating forces to flows with resistance coefficients. 

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