Best Lewis Structure
The Lewis structure that is closest to your structure is determined.
The hybridization of the atoms in this idealized Lewis structure
is given in the table below.
Hybridization in the Best Lewis Structure
1. A bonding orbital for C1-N2 with 1.9942 electrons
__has 41.71% C 1 character in a s0.96 p3 hybrid
__has 58.29% N 2 character in a sp2.67 hybrid
2. A bonding orbital for C1-H3 with 1.9797 electrons
__has 59.83% C 1 character in a s0.96 p3 hybrid
__has 40.17% H 3 character in a s orbital
3. A bonding orbital for C1-H4 with 1.9808 electrons
__has 59.82% C 1 character in a s0.97 p3 hybrid
__has 40.18% H 4 character in a s orbital
4. A bonding orbital for C1-H5 with 1.9967 electrons
__has 60.05% C 1 character in a sp2.68 hybrid
__has 39.95% H 5 character in a s orbital
5. A bonding orbital for N2-O6 with 1.9962 electrons
__has 44.15% N 2 character in a sp2.63 hybrid
__has 55.85% O 6 character in a sp2.62 hybrid
6. A bonding orbital for N2-O6 with 1.9913 electrons
__has 37.97% N 2 character in a p-pi orbital ( 99.51% p 0.49% d)
__has 62.03% O 6 character in a p-pi orbital ( 99.79% p 0.21% d)
10. A lone pair orbital for N2 with 1.9826 electrons
__made from a sp1.15 hybrid
11. A lone pair orbital for O6 with 1.9923 electrons
__made from a sp0.47 hybrid
12. A lone pair orbital for O6 with 1.9646 electrons
__made from a s0.16 p3 hybrid
-With core pairs on: C 1 N 2 O 6 -
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Donor Acceptor Interactions in the Best Lewis Structure
The localized orbitals in your best Lewis structure
can interact strongly. A filled bonding or lone pair orbital can
act as a donor and an empty or filled bonding, antibonding, or
lone pair orbital can act as an acceptor. These
interactions can strengthen and weaken bonds. For example, a
lone pair donor->antibonding acceptor orbital interaction
will weaken the bond
associated with the antibonding orbital. Conversly, an interaction
with a bonding pair as the acceptor will strengthen the bond.
Strong electron delocalization in your best Lewis structure will
also show up as donor-acceptor interactions.
Interactions greater than 20 kJ/mol for bonding and lone pair
orbitals are listed below.
The interaction of bonding donor orbital, 2, for C1-H3 with
the second antibonding acceptor orbital, 90, for N2-O6 is 26.1 kJ/mol.
The interaction of bonding donor orbital, 3, for C1-H4 with
the second antibonding acceptor orbital, 90, for N2-O6 is 24.2 kJ/mol.
The interaction of the second lone pair donor orbital, 12, for O6 with
the antibonding acceptor orbital, 85, for C1-N2 is 73.4 kJ/mol.
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Molecular Orbital Energies
The orbital energies are given in eV, where 1 eV=96.49 kJ/mol.
Orbitals with very low energy are core 1s orbitals.
More antibonding orbitals than you might expect are sometimes
listed, because d orbitals are always included for heavy
atoms and p orbitals are included for H atoms.
Up spins are shown with a ^ and down spins are shown as v.
16 ----- 3.049
15 ----- 2.006
14 ----- 1.454
13 ----- -3.985
12 -^-v- -5.199
11 -^-v- -9.326
10 -^-v- -9.938
9 -^-v- -11.75
8 -^-v- -12.12
7 -^-v- -12.16
6 -^-v- -15.19
5 -^-v- -19.80
4 -^-v- -28.93
3 -^-v- -267.3
2 -^-v- -380.5
1 -^-v- -508.1
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Total Electronic Energy
The total electronic energy is a very large number, so by convention
the units are given in atomic units, that is Hartrees (H). One
Hartree is 2625.5 kJ/mol. The energy reference is for totally
dissociated atoms. In other words, the reference state is a gas
consisting of nuclei and electrons all at infinite distance from
each other. The electronic energy includes all electric
interactions and the kinetic energy of the electrons. This energy
does not include translation, rotation, or vibration of the
the molecule.
Total electronic energy = -169.8636658968 Hartrees
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