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7<br />
5 b.) continued<br />
The third MO (which is unoccupied) is defined by the expression<br />
φ 3 = c 13 f 1 + c 23 f 2 + c 33 f 3<br />
= 0.0 f 1sLi − 0.820 f 2sLi + 0.493 f 1sH .<br />
Here, we see that, like the second MO, the third MO consists of a combination of the 2s valence orbital on<br />
Li and the 1s valence € orbital on H, φ 3 = −0.820 f 2sLi + 0.493 f 1sH . This appears to be an antibonding MO;<br />
since one coefficient is positive and the other is negative, the atomic orbitals subtract to form an<br />
antibonding MO with a node along the internuclear axis.<br />
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c.) The molecular orbital energies are ε 1 = –2.426 a.u., ε 2 = –0.618 a.u., and<br />
a.u. Do these results agree qualitatively with what you would expect<br />
ε 3 = 0.085<br />
The energies of the AOs in atomic units are<br />
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ε 1sLi = − 2.478<br />
ε 2sLi = − 0.196<br />
ε 1sH = − 0.500.<br />
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What do these atomic orbital energies suggest about the AOs that mix to form MOs<br />
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We might expect the first MO, which represents something closely resembling the core 1s orbital on Li, to<br />
be much lower in energy than the second MO, which represents the bonding MO. This is why we say that<br />
the core atomic orbitals do not contribute to the bonding – they are generally too low in energy to<br />
effectively combine with the valence atomic orbitals to form the bonds. Since MO1 consists solely of the<br />
core 1s atomic orbital on Li, we would expect that the orbital energy of MO1 would be nearly the same as<br />
the energy of the 1s atomic orbital, and it is. It is also much lower in energy than the other AOs or MOs.<br />
We also would generally expect a bonding MO to have an orbital energy that is less than zero. A negative<br />
orbital energy generally indicates a favorable interaction (since it is dominated by the Coulomb interaction,<br />
which is negative in sign for an attractive interaction). The second MO consists of a linear combination of<br />
the 2s orbital on Li and the 1s orbital on H, forming a bonding orbital. The energy of this MO is similar<br />
to the energies of the two atomic orbitals from which it is formed, but the MO energy is a bit lower due to<br />
the favorable bonding interaction, so this also makes sense.<br />
Finally, we would expect an antibonding MO to have an orbital energy that is greater than zero. A positive<br />
orbital energy generally indicates an unfavorable interaction. The third MO consists of a linear combination<br />
of the 2s orbital on Li and the 1s orbital on H, forming an antibonding orbital. The energy of this MO is<br />
higher than the energies of the two atomic orbitals from which it is formed, so this also makes sense.<br />
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