i) G is defined as H−TS where H and S are enthalpy and entropy of the system respectively T= temperature. Since H and S are state functions, G is a state function.
ii) G is an extensive property while ΔG=G2−G1 which is the free energy change between the initial and final states of the system.
iii) G has a single value for the thermodynamic state of the system.
iv) G and ΔG value correspond to the system only.
There are three cases of ΔG in predicting the nature of the process.
a) When ΔG<0, (Negative), the process is spontaneous and feasible.
b) When ΔG=0, the process is in equilibrium.
c) When ΔG>0, (Positive), the process is non-spontaneous and not feasible.
v) ΔG=ΔH−TΔS but according of I law of thermodynamics.
ΔH=ΔE+PΔV and ΔE=q−w
∴ΔG=q−w+PΔV−TΔS
but ΔS−q/T and TΔS=q= heat involved in the process.
∴ΔG=q−w+PΔV−q=w+PΔV
(or) −ΔG=w−PΔV= Network.
The decrease in free energy −ΔG, accompanying a process taking place at constant temperature and pressure is equal to maximum obtainable work.
Network =−ΔG=w−PΔV