“…It becomes immediately obvious that, the first contribution embodies direct microstructural information on the system at the ground state, while the second contribution represents an integral over the difference of microstructural behavior between the activated state and the ground state of the viscous flow. In fact, this feature leads to the following equivalent expression to eq , B i ( T , P ) = ν z j o false( υ j o scriptS i j ∞ − υ j ‡ , o scriptS i j , η ‡ , ∞ false) ̅ + ν υ j o scriptS i j ∞ where z j o = β P υ j o identifies the compressibility factor of the pure j –solvent at the prevailing ( T , P ) state conditions, and false( υ j o scriptS i j ∞ − υ j , η ‡ , o scriptS i j , η ‡ , ∞ false) ̅ P − 1 ∫ 0 P ( υ ...…”