3. Larger Molecules The group
orbitals introduced in Chap. 2 and used to interpret structures using
Walsh diagrams also form an ideal basis for building up
and understanding the MOs of large molecules. This will
be demonstrated for several examples below, but before
discussing the examples in detail, we should consider the
two alternative approaches to understanding molecular
structures and reactivity, molecular orbital- and valence bond- (VB) theory. The MO- and
VB- approaches are alternative ways to look at the
same problem - chemical bonding. This is unfortunately
not always made completely clear in organic or inorganic
textbooks, but rather the two approaches are used side by
side without any consideration of their relationship to
each other. Often, chemists use the treatment that is
best suited for the problem in hand. It is, for instance,
very difficult to find a molecular orbital description of
an aldol condensation in current textbooks, whereas the
stereoselectivity of electrocyclic reactions is usually discussed using
MO-theory. This is because an aldol condensation, which
can be treated using MO-theory, can be described much
more succinctly using typical "arrow pushing"
(i.e. VB) arguments:
An
electrocyclic reaction, on the other hand, can be
depicted using a VB-picture, but its stereochemistry
cannot be deduced from such a treatment:
Generally, a
VB-treatment is used to teach chemistry (because it is
more succinct and less complicated than MO-theory) until
cases (like electrocyclic reactions) are treated that
cannot be understood properly within simple VB-theory.
This need not be the case, but is usually a good
compromise for teaching chemical bonding and reactivity
effectively. There is,
however, one quantity, atomic charge, that has very
different meanings within the two theories. Simple
VB-theory uses Lewis
structures
to describe the bonding in molecules. Formal Lewis
charges are assigned in order to complete the octet of a
given atom, but do not indicate that the atom in question
actually has the formal charge (atomic charges are not
physically measurable quantities, but can be assigned by
a variety of analyses within MO-theory). Take, for
instance, the pyridinium and tetramethylammonium cations:
The nitrogen is the most electronegative atom in these ions, so that it is the last place that we would expect to find a positive charge. In fact, whichever method we use to calculate the atomic charges, the nitrogens turn out to be slightly negative. The positive charge in the tetramethylammonium ions is almost completely situated on the 12 hydrogens. We will now
treat some common molecules using qualitative MO-theory.
It is, however, important to remember that this treatment
is an alternative to the common Lewis (VB) picture. We
will point out some of the differences for the individual
molecules. |