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in less than 1 minute on a laptop relatively far from nuclei (note scale of bond lengths) |
when it was a real accomplishment using room-filling computers at a higher value of psi; closer to nuclei |
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mostly 2pC antibonding with a little 2pF makes C-Halogen a functional group |
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p HOMOs antibonding between 2pF and sCH |
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2pF s AO bonding to C or sCH)
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p MOs 2pF and sCH
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overlapping favorably with a little of 2pF |
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modest bonding contribution from C |
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Organic Chemist's Book of Orbitals Academic Press, 1973 |
It is fun to find the nodes in these MOs, and to rationalize, in retrospect, what went into each of them and why. But it is not so easy to predict their exact shape without a computer, so if this look almost impossibly challenging, don't feel that your missing something important, humans can do it reliably in their head.
Fortunately, we don't really care about the shape of most MOs - only the LUMO (and/or HOMO), and even then only when it is unusually low (or high) in energy. These "frontier orbitals" are the only ones whose energy-match with orbitals from other molecules is good enough to make them relevant to reactivity.
High Unoccupied MOs are irrelevant, because electrons will never go there. Low Occupied MOs are nearly irrelevant, because their energy match with UMOs is too poor for them to be involved in reaction - as a set they are just one way to carve up the pie of molecular electron density into cognitively bite-sized portions. There are other ways.
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