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The geometry optimizations for the three highest level of theory
are shown. The bond angle of oxygen is 180 degrees and not
included for this report. The literature value for the bond
length of oxygen was 1.2075 angstroms.
2 The
calculated values for each theory were the same and gave an
error of 6.00%.
6-21G was the lowest level of theory used for geometry
optimization.
6-31G was the next highest level of theory for geometry
optimization.
Double Zeta Valence was the highest level of theory used for
geometry optimization.
This is the highest occupied molecular orbital at orbital eight.
The orbitals were determined by totaling the number of electron
in the molecule and dividing by two.
This is the lowest occupied molecular orbital at orbital nine.
This orbital would be the next occupied if the molecule were
excited with an adequate amount of energy.
The partial atomic charge for a diatomic molecule is zero, which
is shown here. They are created by the asymmetric distribution
of electrons in a chemical bond; diatomic molecules have
symmetric distributions because of equivalent
electronegativities.
Table and Figure 1 below show the different orbitals for the O
2
molecule starting with the S sigma bonding orbitals and going
down to the highest energy orbitals. The two P orbitals
represent the p
x and p
y orbitals that
contribute to pi bonding.
Figure 1: Orbital diagram showing the participating
atomic orbitals from each oxygen atom, the molecular orbitals
that result from their overlap, and the Aufbau filling of the
orbitals.
3
Table 1: Orbitals corresponding to the type of bonding
occurring at that level.
Type of Bonding
|
Orbital
|
S sigma bonding
|
|
S sigma anti-bonding
|
|
P bonding
|
|
P anti-bonding
|
|
P2 bonding |
|
P2 anti-bonding |
|
The different potential energies of bond stretching at different
levels of theory are shown in Figure 1. The higher the level of
theory, the lower in energy the theory calculates for the lowest
potential energy. The bump in the graph is due to the
interactions between electrons that are not accounted for in the
theories. An experimental graph of potential energy would not
have these bumps.
Figure 2: Potential energy (Hartrees) curves at different
levels of theory plotted against bond lengths (angstroms).
4
The vibrational frequency using DZV theory was 1364.52 cm
-1.
In comparison to the NIST database value, 1580 cm
-1,
there was a 13.6% error.
2
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