A wide array of organic molecules exhibit delocalized bonding. Benzene is the most famous example, but modern understanding has revealed that electron delocalization is a very important feature of many systems.
Molecular orbital theory offers some obvious advantages for explaining delocalized bonding. However, if we properly understand the background of VB theory, we can use the simple method of using bond-line structures to convey concepts that otherwise require numerical analysis of MO calculations.
Consider, for example, the allyl cation. Ignoring the sigma framework for the moment, we find that three p orbitals can interact to form 3 molecular orbitals, shown here in descending order of their energy:
Load the frontier molecular orbitals to visualize the π bonding: Show the antibonding MO (empty) Show the nonbonding MO (empty in the cation) Show the bonding π MO (filled--occupied by 2 electrons) |
(There are, of course, additional MOs arising from the sigma framework.)
The lowest energy orbital will have 2 electrons, and the other two are empty "virtual" orbitals. We can extract two important features from this picture:
The same conclusions can be drawn from the proper use of resonance forms:
The proper interpretation of this diagram is that:
The picture we draw is effectively identical to that arising from MO theory. Use of the resonance forms provides a concise way to convey the same thing as the MO drawings, but is quicker to use and easier (in most cases) to interpret. There are situations where use of resonance structures is inadequate; in these cases a more quantitative picture may be developed using molecular orbital computations.
Rules for Writing and Interpreting Resonance Structures
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Last updated: 09/21/2000