c21 JWBS043-Rogers September 13, 2010 11:30 Printer Name: Yet to Come
350 PHOTOCHEMISTRY AND THE THEORY OF CHEMICAL REACTIONS
rHH. At some instant, the incoming H and the departing H must be equidistant from
the central hydrogen atom so that the three atoms form an energetic intermediate:
H+H−H=
⎡
⎣H
r′HH
︷︸︸︷
···H
rHH
︷︸︸︷
···H
⎤
⎦=H−H+H
Thebond-formingconfiguration is on the left and thebond-breakingconfiguration is
on the right of the central structure, which is theactivated complex.
21.7 THE POTENTIAL ENERGY SURFACE
In the study of molecular structure, we plotted the potential energy of the molecule as
a function of internuclear distance and found that it has a minimum at the equilibrium
bond length. Some of the qualities of this potential energy curve carry over to the
activated complex, but now the potential energy is a more complicated function of two
variablesr′HHandrHH. It requires a three-dimensional surface or a two-dimensional
contour map for its representation. Eyring has constructed such a surface represented
by the equivalent contour map in Fig. 21.2.
This contour map is drawn in the same way that a forest service map of Western
Montana would be drawn. Each contour corresponds to a constant potential energy
that would occupy the dimension out of the plane of the paper if the three-dimensional
representation were used. The hyperbola connecting the two arrows is the locus of
potential energy minima of the system as the reaction takes place. Contour 4 bounds
a potential energy plateau.
rHH
r'HH
V
1
2
3
4
FIGURE 21.2 Eyring potential energy plot for the reaction H+H H→H H+H.