Jump to
S1C2
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -167.671515 |
| Energy at 298.15K | |
| HF Energy | -167.671515 |
| Nuclear repulsion energy | 61.516013 |
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 HF/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 |
3664 |
3314 |
279.28 |
8.85 |
0.27 |
0.42 |
| 2 |
Σ |
2507 |
2267 |
405.08 |
83.39 |
0.18 |
0.30 |
| 3 |
Σ |
1315 |
1189 |
287.48 |
4.73 |
0.33 |
0.50 |
| 4 |
Π |
644 |
582 |
10.65 |
3.11 |
0.75 |
0.86 |
| 4 |
Π |
644 |
582 |
10.65 |
3.11 |
0.75 |
0.86 |
| 5 |
Π |
588 |
532 |
76.35 |
3.77 |
0.75 |
0.86 |
| 5 |
Π |
588 |
532 |
76.35 |
3.77 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4974.5 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 4499.0 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 HF/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.165 |
| N2 |
0.000 |
0.000 |
-0.027 |
| C3 |
0.000 |
0.000 |
-1.154 |
| H4 |
0.000 |
0.000 |
-2.208 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1915 | 2.3184 | 3.3725 |
N2 | 1.1915 | | 1.1269 | 2.1811 | C3 | 2.3184 | 1.1269 | | 1.0542 | H4 | 3.3725 | 2.1811 | 1.0542 | |
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 HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.500 |
|
|
|
| 2 |
N |
0.122 |
|
|
|
| 3 |
C |
0.013 |
|
|
|
| 4 |
H |
0.366 |
|
|
|
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 |
-4.279 |
4.279 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.671 |
0.000 |
0.000 |
| y |
0.000 |
-16.671 |
0.000 |
| z |
0.000 |
0.000 |
-13.955 |
|
| Traceless |
| | x | y | z |
| x |
-1.358 |
0.000 |
0.000 |
| y |
0.000 |
-1.358 |
0.000 |
| z |
0.000 |
0.000 |
2.715 |
|
| Polar |
| 3z2-r2 | 5.431 |
| 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 |
1.364 |
0.000 |
0.000 |
| y |
0.000 |
1.364 |
0.000 |
| z |
0.000 |
0.000 |
5.256 |
<r2> (average value of r
2) Å
2
| <r2> |
33.565 |
| (<r2>)1/2 |
5.793 |
Jump to
S1C1
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -167.671515 |
| Energy at 298.15K | -167.672495 |
| HF Energy | -167.671515 |
| Nuclear repulsion energy | 61.518979 |
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 HF/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' |
3665 |
3315 |
279.13 |
|
|
|
| 2 |
A' |
2506 |
2267 |
406.62 |
|
|
|
| 3 |
A' |
1316 |
1190 |
287.37 |
|
|
|
| 4 |
A' |
644 |
583 |
10.42 |
|
|
|
| 5 |
A' |
586 |
530 |
76.66 |
|
|
|
| 6 |
A" |
643 |
581 |
20.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4680.1 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 4232.7 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 HF/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.002 |
-1.165 |
0.000 |
| N2 |
0.000 |
0.027 |
0.000 |
| C3 |
0.002 |
1.154 |
0.000 |
| H4 |
0.005 |
2.208 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1912 | 2.3183 | 3.3723 |
N2 | 1.1912 | | 1.1271 | 2.1811 | C3 | 2.3183 | 1.1271 | | 1.0540 | H4 | 3.3723 | 2.1811 | 1.0540 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.998 |
|
N2 |
C3 |
H4 |
179.958 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.500 |
|
|
|
| 2 |
N |
0.122 |
|
|
|
| 3 |
C |
0.012 |
|
|
|
| 4 |
H |
0.366 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.009 |
4.276 |
0.000 |
4.276 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.671 |
0.008 |
0.000 |
| y |
0.008 |
-13.957 |
0.000 |
| z |
0.000 |
0.000 |
-16.671 |
|
| Traceless |
| | x | y | z |
| x |
-1.357 |
0.008 |
0.000 |
| y |
0.008 |
2.714 |
0.000 |
| z |
0.000 |
0.000 |
-1.357 |
|
| Polar |
| 3z2-r2 | -2.714 |
| x2-y2 | -2.714 |
| xy | 0.008 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.364 |
0.007 |
0.000 |
| y |
0.007 |
5.257 |
0.000 |
| z |
0.000 |
0.000 |
1.364 |
<r2> (average value of r
2) Å
2
| <r2> |
33.563 |
| (<r2>)1/2 |
5.793 |