Jump to
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -168.560735 |
| Energy at 298.15K | |
| HF Energy | -168.560735 |
| Nuclear repulsion energy | 60.880805 |
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 B1B95/6-311G**
| 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 |
3538 |
3397 |
263.07 |
23.19 |
0.24 |
0.39 |
| 2 |
Σ |
2378 |
2283 |
390.06 |
29.53 |
0.13 |
0.23 |
| 3 |
Σ |
1342 |
1289 |
127.83 |
18.98 |
0.29 |
0.45 |
| 4 |
Π |
586 |
563 |
0.22 |
0.60 |
0.75 |
0.86 |
| 4 |
Π |
586 |
563 |
0.22 |
0.60 |
0.75 |
0.86 |
| 5 |
Π |
277 |
266 |
88.50 |
4.33 |
0.75 |
0.86 |
| 5 |
Π |
277 |
266 |
88.50 |
4.33 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4492.5 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 4313.3 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 B1B95/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.173 |
| N2 |
0.000 |
0.000 |
-0.017 |
| C3 |
0.000 |
0.000 |
-1.173 |
| H4 |
0.000 |
0.000 |
-2.231 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1898 | 2.3456 | 3.4041 |
N2 | 1.1898 | | 1.1559 | 2.2143 | C3 | 2.3456 | 1.1559 | | 1.0584 | H4 | 3.4041 | 2.2143 | 1.0584 | |
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 B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.352 |
|
|
|
| 2 |
N |
0.098 |
|
|
|
| 3 |
C |
0.045 |
|
|
|
| 4 |
H |
0.209 |
|
|
|
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 |
-3.104 |
3.104 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.550 |
0.000 |
0.000 |
| y |
0.000 |
-16.550 |
0.000 |
| z |
0.000 |
0.000 |
-13.920 |
|
| Traceless |
| | x | y | z |
| x |
-1.315 |
0.000 |
0.000 |
| y |
0.000 |
-1.315 |
0.000 |
| z |
0.000 |
0.000 |
2.630 |
|
| Polar |
| 3z2-r2 | 5.261 |
| 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 |
1.449 |
0.000 |
0.000 |
| y |
0.000 |
1.449 |
0.000 |
| z |
0.000 |
0.000 |
5.621 |
<r2> (average value of r
2) Å
2
| <r2> |
34.027 |
| (<r2>)1/2 |
5.833 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -168.560737 |
| Energy at 298.15K | -168.561372 |
| HF Energy | -168.560737 |
| Nuclear repulsion energy | 60.877435 |
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 B1B95/6-311G**
| 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' |
3539 |
3398 |
262.83 |
|
|
|
| 2 |
A' |
2379 |
2284 |
390.02 |
|
|
|
| 3 |
A' |
1343 |
1289 |
127.76 |
|
|
|
| 4 |
A' |
587 |
563 |
0.21 |
|
|
|
| 5 |
A' |
276 |
265 |
88.51 |
|
|
|
| 6 |
A" |
583 |
560 |
2.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4352.6 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 4179.0 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 B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.007 |
-1.173 |
0.000 |
| N2 |
0.000 |
0.017 |
0.000 |
| C3 |
0.007 |
1.173 |
0.000 |
| H4 |
0.012 |
2.231 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1898 | 2.3458 | 3.4042 |
N2 | 1.1898 | | 1.1560 | 2.2144 | C3 | 2.3458 | 1.1560 | | 1.0585 | H4 | 3.4042 | 2.2144 | 1.0585 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.977 |
|
N2 |
C3 |
H4 |
179.916 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.352 |
|
|
|
| 2 |
N |
0.098 |
|
|
|
| 3 |
C |
0.045 |
|
|
|
| 4 |
H |
0.209 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.016 |
3.105 |
0.000 |
3.105 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.551 |
0.011 |
0.000 |
| y |
0.011 |
-13.919 |
0.000 |
| z |
0.000 |
0.000 |
-16.551 |
|
| Traceless |
| | x | y | z |
| x |
-1.316 |
0.011 |
0.000 |
| y |
0.011 |
2.631 |
0.000 |
| z |
0.000 |
0.000 |
-1.316 |
|
| Polar |
| 3z2-r2 | -2.632 |
| x2-y2 | -2.631 |
| xy | 0.011 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.449 |
0.025 |
0.000 |
| y |
0.025 |
5.621 |
0.000 |
| z |
0.000 |
0.000 |
1.449 |
<r2> (average value of r
2) Å
2
| <r2> |
34.030 |
| (<r2>)1/2 |
5.833 |