Jump to
S1C2
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -167.747254 |
| Energy at 298.15K | -167.747509 |
| HF Energy | -167.747254 |
| Nuclear repulsion energy | 60.660876 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at LSDA/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3445 |
3403 |
267.50 |
|
|
|
| 2 |
Σ |
2351 |
2322 |
327.30 |
|
|
|
| 3 |
Σ |
1344 |
1327 |
80.53 |
|
|
|
| 4 |
Π |
573 |
566 |
0.22 |
|
|
|
| 4 |
Π |
573 |
566 |
0.22 |
|
|
|
| 5 |
Π |
154 |
152 |
91.97 |
|
|
|
| 5 |
Π |
154 |
152 |
91.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4297.3 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 4244.4 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at LSDA/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.175 |
| N2 |
0.000 |
0.000 |
-0.012 |
| C3 |
0.000 |
0.000 |
-1.179 |
| H4 |
0.000 |
0.000 |
-2.248 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1874 | 2.3541 | 3.4233 |
N2 | 1.1874 | | 1.1667 | 2.2359 | C3 | 2.3541 | 1.1667 | | 1.0692 | H4 | 3.4233 | 2.2359 | 1.0692 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
180.000 |
|
N2 |
C3 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.290 |
|
|
|
| 2 |
N |
0.075 |
|
|
|
| 3 |
C |
0.002 |
|
|
|
| 4 |
H |
0.214 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-2.719 |
2.719 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.747 |
0.000 |
0.000 |
| y |
0.000 |
-16.747 |
0.000 |
| z |
0.000 |
0.000 |
-13.974 |
|
| Traceless |
| | x | y | z |
| x |
-1.387 |
0.000 |
0.000 |
| y |
0.000 |
-1.387 |
0.000 |
| z |
0.000 |
0.000 |
2.774 |
|
| Polar |
| 3z2-r2 | 5.547 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.498 |
0.000 |
0.000 |
| y |
0.000 |
1.498 |
0.000 |
| z |
0.000 |
0.000 |
5.705 |
<r2> (average value of r
2) Å
2
| <r2> |
34.324 |
| (<r2>)1/2 |
5.859 |
Jump to
S1C1
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -167.747254 |
| Energy at 298.15K | -167.747699 |
| HF Energy | -167.747254 |
| Nuclear repulsion energy | 60.660078 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at LSDA/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3445 |
3403 |
267.48 |
|
|
|
| 2 |
A' |
2351 |
2322 |
327.27 |
|
|
|
| 3 |
A' |
1344 |
1327 |
80.53 |
|
|
|
| 4 |
A' |
573 |
566 |
0.22 |
|
|
|
| 5 |
A' |
154 |
152 |
91.97 |
|
|
|
| 6 |
A" |
573 |
566 |
0.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4220.3 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 4168.4 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at LSDA/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.011 |
-1.175 |
0.000 |
| N2 |
0.000 |
0.012 |
0.000 |
| C3 |
0.011 |
1.179 |
0.000 |
| H4 |
0.019 |
2.248 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1874 | 2.3541 | 3.4233 |
N2 | 1.1874 | | 1.1667 | 2.2359 | C3 | 2.3541 | 1.1667 | | 1.0692 | H4 | 3.4233 | 2.2359 | 1.0692 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.965 |
|
N2 |
C3 |
H4 |
179.823 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.290 |
|
|
|
| 2 |
N |
0.075 |
|
|
|
| 3 |
C |
0.002 |
|
|
|
| 4 |
H |
0.214 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.021 |
2.719 |
0.000 |
2.719 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.747 |
0.017 |
0.000 |
| y |
0.017 |
-13.974 |
0.000 |
| z |
0.000 |
0.000 |
-16.747 |
|
| Traceless |
| | x | y | z |
| x |
-1.387 |
0.017 |
0.000 |
| y |
0.017 |
2.774 |
0.000 |
| z |
0.000 |
0.000 |
-1.387 |
|
| Polar |
| 3z2-r2 | -2.774 |
| x2-y2 | -2.774 |
| xy | 0.017 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.498 |
0.040 |
0.000 |
| y |
0.040 |
5.705 |
0.000 |
| z |
0.000 |
0.000 |
1.498 |
<r2> (average value of r
2) Å
2
| <r2> |
34.325 |
| (<r2>)1/2 |
5.859 |