Solution Thermodynamics

· This week we will be principally reviewing the interrelationships present between the various properties we use to describe mixtures

· Towards the end of class there should also be time to review some solutions to problems from the textbook

1. Fugacity and Partial Molar Properties

We given definitions for both component and mixture fugacity:

If we integrate both from the ideal-gas state (where and ) to the real-gas state:

If we take the partial molar property of this latter equation we get:

There are two possible rearrangements of this:

Or:

From the first rearrangement we find that:

 

From the second rearrangement we find that:

If these quantities are partial molar properties, it thus follows that:

And that:

2. Shape of Fugacity vs Composition Curve

One example of the significance of the Gibbs-Duhem equation is the insight it gives us as to the shape of the fugacity curve:

For a binary mixture (), we get:

Or:

If we take the limit as x1® 1, x2® 0 we find:

Or:

Thus the fugacity vs. composition curve is tangent to the Lewis-Randall line () as x1® 1:

3. Dependence of f and f on T and P

We begin with the definition of fugacity:

and integrate from the ideal-gas state to real-gas state:

 

But by the Gibbs-Helmholtz Equation:

Thus:

For the pressure dependence, we again use the definition of fugacity:

Giving:

Or:

Thus:

· These represent the fundamental property relations for f and f

· Unfortunately, we're generally more interested in and than we are in f and f

4. Dependence of and on T and P

Consider a constant-composition mixture:

We take the partial molar property of each term:

But , and is constant:

Similarly,

Leads to:

Or:

5. Property Change of Mixing

Is defined as:

where

M = property of mixture (at some T and P)

= property of pure i (in its standard state)

Notes

· Since

· This suggests that . Can verify:

Thus we can write for the various properties:

 

But we recall the following relationships:

Thus:

6. Activity

Obviously, the quantity () is important. We can evaluate it using the definition of fugacity:

We now define the activity as this fugacity ratio:

We can once again re-write the expressions for the property changes of mixing:

7. Ideal Solution

We now define the concept of an ideal solution:

For an ideal solution we have:

8. Excess Properties

Mixture properties are usually evaluated by reference to the property of the ideal mixture:

where M = the actual property of mixture

Mid = the property of an ideal mixture

ME, M and Mid are all at the same T,P & x

Note that Mid, and thus ME, depends on choice of

standard states

The quantity "M" could refer to any intensive thermodynamic property, including a property change of mixing:

Thus we conclude that the excess property change of mixing and the excess property are exactly the same quantity:

However, D M and D Mid are easier to evaluate in most cases, thus in practice we use the relation:

Recall that D Mid=0 for U, H, V, CP, and CV, thus:

Thus we can write:

Or:

Similarly, we write for the other excess properties:

 

 

9. Activity Coefficient

Clearly the ratio of the activity to the mole fraction is an important quantity; we thus define it as the activity coefficient:

Of course, each of the excess property expressions can now be re-written in terms of the activity coefficient:

Of these excess properties, we are particularly interested in the excess Gibbs energy. Let's find the partial molar property corresponding to it:

But, using the definition of component fugacity:

Thus:

Or:

We see that is the partial molar property of GE/RT.

 

10. Excess Gibbs Energy and Fugacity

As we have seen,

Since the first term is of the form :

We find that:

And since:

11. Activity as a Partial Molar Property

Among our relations for excess properties we saw:

Thus:

But:

So:

 

12. Gibbs-Duhem Equations for D G and GE

We can now write a fundamental property relation for D G:

Or:

And the corresponding Gibbs-Duhem Equation is:

In similar fashion, a general property relation for GE is:

And the corresponding Gibbs-Duhem Equation is:

13. Dependence of Activity Coefficient on T & P

Note that these last expressions give, in the style of the Maxwell Relations:

And:

 

Main Points Reviewed This Week

1. Fugacity and Partial Molar Properties

2. Shape of Fugacity vs Composition Curve

3. Dependence of f and f on T and P

4. Dependence of and on T and P

5. Property Change of Mixing

6. Activity

7. Ideal Solution

 

8. Excess Properties

9. Activity Coefficient

10. Excess Gibbs Energy and Fugacity

11. Activity as a Partial Molar Property

12. Gibbs-Duhem Equations for D G and GE

13. Dependence of Activity Coefficient on T & P