COUPLED TRANSPORT CAN BE DESCRIBED BY NON-EQUILIBRIUM THERMODYNAMICS

• THERMODYNAMICS OF THE STEADY STATE

PHENOMENOLOGICAL EQUATIONS:

J1 = L11 X1 + L12 X2

J2 = L21 X1 + L22 X2

DISSIPATION FUNCTION:

T dS/dt = J1 X1 + J2 X2

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