Urmi Roy said:
How can we use this paragraph to explain the equation : F = C − P + 2 ,
and explain how Gibbs reasoned this out?
Keep in mind that's not exactly correct. Chemical equiibrium poses additional constraints, so it's actually F=C-P-R+2.
Let's start out considering the simplest system, which would have one component and only one phase.
The chemical potential is a function of temperature and pressure, regardless of what the equation of state is for that phase.
Now consider what happens when you increase the number of phases: The chemical potential of the substance has to be the same at equilibrium, so we have the constraint {\mu_a}(T,P)={\mu_b}(T,P), or \Delta\mu_{ab}(T,P)={\mu_a}(T,P)-{\mu_b}(T,P)=0. We can choose either T or P as an independent variable, but we can only choose one of them--the new constraint makes the other a dependent variable by default.
Now if we make a third phase
Likewise adding a third phase gives a second delta:
{\mu_a}(T,P)={\mu_c}(T,P) gives us \Delta\mu_{ac}(T,P)={\mu_a}(T,P)-{\mu_c}(T,P)=0. This gives us a different curve on a T,P graph, which will intersect the first curve at a single point if all three phases coexist at once. (or won't intersect at all if the three phases can't coexist)
At this point you're probably wondering why I don't use a third delta:
{\mu_b}(T,P)={\mu_c}(T,P) gives us \Delta\mu_{bc}(T,P)={\mu_b}(T,P)-{\mu_c}(T,P)=0. But notice that \Delta\mu_{bc}(T,P)={\mu_b}(T,P)-{\mu_a}(T,P)-{\mu_c}(T,P)+{\mu_a}(T,P)=\Delta\mu_{ac}(T,P)-\Delta\mu_{ab}(T,P)--so this third delta is simply a combination of the other two.
Mathematically it will always be zero when both of the others are.
Now let's go back to the one-phase system, but add a second component.
Now we have the chemical potential of each substance as a function of three independent variables: temperature, pressure, and mole fraction of component #1. We could also use the mole fraction of component #2, but {X_1}+{X_2}=1 so only one mole fraction is an independent variable.