We saw two simple MO diagrams in the section on H2. Now let's think about how to make
some slightly more complicated MO diagrams. First, we need to know a
little about how big the energy splitting
between the bonding and anti-bonding MOs is. Splitting is the energy
difference between the bonding and anti-bonding orbitals. Usually the
bonding orbital goes down almost as much as the antibonding orbital goes up,
so the average energy stays almost the same. The size of the splitting
depends on the energy match and the overlap.
Energy match means how close the orbital
energies are. The reason we can consider only valence orbitals is that
the core orbitals have much lower energy, and the higher empty
orbitals have much higher energy, than the valence
electrons. Interactions between completely completely empty
orbitals don't matter because there are no electrons. Interactions
between completely filled orbitals are usually repulsive, which is why
the noble gases don't usually make bonds. Interactions between
partially-filled valence orbitals and either core orbitals or higher
shell orbitals aren't important because the energy match is bad, so
the splitting is almost zero.
We talked about overlap a little in the previous
section. Overlap means how much the orbitals touch. For example,
usually σ combinations have bigger overlap than π
combinations, because the orbitals are pointed right toward each
other. You can see this in the pictures on the previous page. For this
reason, usually σ MOs have bigger splitting than π MOs.
MO diagram for HF
In the last section, we talked about the bonding, non-bonding, and
anti-bonding MOs in HF. Now let's put these ideas together to make an
MO diagram for HF.
We need to know what orbitals we are using. We are only going to
consider valence orbitals. H has a 1s orbital. F has a 2s orbital
and 3 2p orbitals (x,y,z).
We want to know the energies of the orbitals. We can use
photoelectron spectroscopy data, which tells us the energy of the
different orbitals. Here
is some data you can use. We see that H 1s orbital has energy -13.6
eV, F 2s has energy -40 eV and F 2p has energy -18.7 eV. Because
there is a big energy difference, more than 12eV, between H 1s and F 2s (bad energy
match), we can put just H 1s and F 2p in our diagram.
We draw the AOs on the outside of the diagram and include
the right number of electrons. H has 1 valence electron, and F has 7
valence electrons. We are only including the F 2p orbitals, which
have 5 electrons; the F 2s orbital holds 2 electrons and isn't in
the diagram (it's like a lone pair).
We remember which orbitals interact. Before, we saw that bonding
and antibonding combinations only form between H 1s and the F 2p
orbital that points straight toward it. The other 2p orbitals are
non-bonding, so we can draw them in the middle at the same starting
energy.
The H 1s and F 2pz make a bonding and anti-bonding
combination, so we draw these new MO energy levels. We don't know
exactly how big the splitting is, but that's ok, don't worry about
it.
We put the same number of valence electrons we had in the AOs on
the outside
into the MOs at the center, starting at the bottom. In this case, we have 6 electrons. They
will go into the bonding MO and the 2 non-bonding MOs. The
antibonding MO is empty because it is too high in energy. We're
done!
MO diagram for F2
Let's do another example. This time we'll do F2, which
is a little more complicated. This time we'll use σ and π
bonds.
What orbitals we are using? F has a 2s orbital
and 3 2p orbitals (x,y,z). For now, let's just consider the 2p
orbitals. We'll see what happens with 2s orbital in the next section.
We don't need to worry about the energies this time, because
they all start the same.
We draw the AOs on the outside of the diagram and include
the right number of electrons. F has 7
valence electrons. We are only including the F 2p orbitals, which
have 5 electrons; the F 2s orbital holds 2 electrons and isn't in
the diagram yet.
We remember which orbitals interact. Before, we saw that we make
σ bond and anti-bonding combinations using the 2p orbitals
that point toward each other. Let's draw those in.
We also make π bonding and
antibonding combinations using the other 2p orbitals. Because these
have less overlap than the σ combinations, the splitting will
be smaller, so we'll draw these in between the σ bonding and
antibonding orbitals. There are 2 of
each (π bonding and antibonding), so we draw 2 lines for each. They are the same energy because the are the same
except rotated 90°.
We put the same number of valence electrons we had in the AOs on
the outside
into the MOs at the center. In this case, we have 10 electrons. They
will go into the σ bonding MO and all 4 π MOs. Only the
σ* MO is left empty. We're
done!
Reading MO diagrams
When you look at an MO diagram, you can see what AOs are included
by checking the outside of the diagram. The middle shows you how
they combine and approximately what the energies of the combinations
are. You can tell which orbitals are bonding because they have lower
energy than the AOs. Non-bonding orbitals have about the same energy
as the AOs, and anti-bonding orbitals have higher energy than the
AOs. You can use the number of electrons in each type of MO to find
the bond order. You can also tell how many unpaired electrons there
are, which tells you about the magnetic properties. You can make
some guesses about colors, because these usually come from having a
small gap between full and empty orbitals. Finally, you can
tell which parts of the molecule are most reactive: they will have a
low-energy empty MO or a high-energy full MO. We'll see some more
examples of this later.