版权所有：华东理工大学物理化学教研室 11 4) The general case of a reaction It follows that r C D BA Δ G = cμ + dμ − aμ − bμ ⎟⎟⎠⎞ ⎜⎜⎝⎛ = ba dc aa aa Q BA DC 9.1 The Gibbs energy minimum C D A B r BADC ln ln ln ln Δ abRTaaRTadRTacRT badcG + + − − −−+= oooo μμμμ Since JJ J += ln aRT o μμ ⎟⎟⎠⎞ ⎜⎜⎝⎛ += ba dc aa aa RTGG BA DC rr ΔΔ ln o版权所有：华东理工大学物理化学教研室 11 4) The general case of a reaction It follows that r C D BA Δ G = cμ + dμ − aμ − bμ ⎟⎟⎠⎞ ⎜⎜⎝⎛ = ba dc aa aa Q BA DC 9.1 The Gibbs energy minimum C D A B r BADC ln ln ln ln Δ abRTaaRTadRTacRT badcG + + − − −−+= oooo μμμμ Since JJ J += ln aRT o μμ ⎟⎟⎠⎞ ⎜⎜⎝⎛ += ba dc aa aa RTGG BA DC rr ΔΔ ln o