c08 JWBS043-Rogers September 13, 2010 11:25 Printer Name: Yet to Come
DEGENERACY AND EQUILIBRIUM 109
A(g) B(g)
· · · εB
· · · · · εA
FIGURE 8.1 A two-level equilibrium. There are 5 molecules in A and 3 molecules in B.
Conversely, knowing the energy separation, one can calculate the equilibrium
constant. If the energy of B islowerthan the energy of A by 2. 10 × 10 −^21 J, level B
will contain more molecules at equilibrium than will level A andKeqwill be larger
than 1.0 (Fig. 8.2).
Keq=
nB
nA
=e−(εB−εA)/kBT=
5
3
= 1. 67
In these simple models, the equilibrium constants are inverses and(εB−εA)of the
first equilibrium is equal but opposite in sign to(εB−εA)of the second reaction. This
analysis gives a description of the relationship between energy and the equilibrium
constant that is useful as far as it goes, but it has left out an important consideration:
the influence of entropy.
8.2 DEGENERACY AND EQUILIBRIUM
If the upper level is split into two levels, each of which has the same energy, its
capacity to accommodate molecules of kind B is doubled (Fig. 8.3). The equilibrium
constantKeq=
6
5
has been made greater than 1.0. The reaction now favors products
rather than reactants even though the energy change is uphill. The second law has
come into play; the product state is more disordered. There are more places for the
molecule to go. It is like having two stacks of paper on your desk rather than one.
There are now two places where that important piece of paper you are looking for may
be, whereas before there was only one. Increased disorder means increased entropy.
· · ·
· · · · ·
A B
FIGURE 8.2 A two-level equilibrium.