Jump to
S1C2
Energy calculated at B3PW91/6-31G**
| hartrees |
Energy at 0K | -168.507708 |
Energy at 298.15K | |
HF Energy | -168.507708 |
Nuclear repulsion energy | 60.364733 |
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 B3PW91/6-31G**
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 |
3544 |
3397 |
252.00 |
|
|
|
2 |
Σ |
2385 |
2286 |
316.47 |
|
|
|
3 |
Σ |
1336 |
1280 |
106.21 |
|
|
|
4 |
Xpi |
576 |
552 |
0.18 |
|
|
|
4 |
Xpi |
576 |
552 |
0.18 |
|
|
|
5 |
Xpi |
224 |
214 |
92.73 |
|
|
|
5 |
Xpi |
224 |
214 |
92.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4431.9 cm
-1
Scaled (by 0.9584) Zero Point Vibrational Energy (zpe) 4247.5 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 B3PW91/6-31G**
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
1.184 |
N2 |
0.000 |
0.000 |
-0.019 |
C3 |
0.000 |
0.000 |
-1.182 |
H4 |
0.000 |
0.000 |
-2.245 |
Atom - Atom Distances (Å)
|
O1 |
N2 |
C3 |
H4 |
O1 | | 1.2023 | 2.3662 | 3.4289 |
N2 | 1.2023 | | 1.1639 | 2.2266 | C3 | 2.3662 | 1.1639 | | 1.0627 | H4 | 3.4289 | 2.2266 | 1.0627 | |
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 B3PW91/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.471 |
|
|
|
2 |
N |
0.180 |
|
|
|
3 |
C |
0.033 |
|
|
|
4 |
H |
0.258 |
|
|
|
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 |
-3.095 |
3.095 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.390 |
0.000 |
0.000 |
y |
0.000 |
-16.390 |
0.000 |
z |
0.000 |
0.000 |
-13.453 |
|
Traceless |
| x | y | z |
x |
-1.469 |
0.000 |
0.000 |
y |
0.000 |
-1.469 |
0.000 |
z |
0.000 |
0.000 |
2.938 |
|
Polar |
3z2-r2 | 5.875 |
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 |
1.352 |
0.000 |
0.000 |
y |
0.000 |
1.352 |
0.000 |
z |
0.000 |
0.000 |
5.459 |
<r2> (average value of r
2) Å
2
<r2> |
34.267 |
(<r2>)1/2 |
5.854 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G**
| hartrees |
Energy at 0K | -168.507708 |
Energy at 298.15K | -168.508167 |
HF Energy | -168.507708 |
Nuclear repulsion energy | 60.367632 |
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 B3PW91/6-31G**
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 |
3545 |
3397 |
251.99 |
|
|
|
2 |
Σ |
2385 |
2286 |
316.82 |
|
|
|
3 |
Σ |
1337 |
1281 |
106.06 |
|
|
|
4 |
Π |
576 |
552 |
0.18 |
|
|
|
4 |
Π |
576 |
552 |
0.18 |
|
|
|
5 |
Π |
223 |
214 |
92.76 |
|
|
|
5 |
Π |
223 |
214 |
92.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4432.1 cm
-1
Scaled (by 0.9584) Zero Point Vibrational Energy (zpe) 4247.7 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 B3PW91/6-31G**
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
-1.184 |
N2 |
0.000 |
0.000 |
0.018 |
C3 |
0.000 |
0.000 |
1.182 |
H4 |
0.000 |
0.000 |
2.245 |
Atom - Atom Distances (Å)
|
O1 |
N2 |
C3 |
H4 |
O1 | | 1.2021 | 2.3661 | 3.4288 |
N2 | 1.2021 | | 1.1639 | 2.2267 | C3 | 2.3661 | 1.1639 | | 1.0628 | H4 | 3.4288 | 2.2267 | 1.0628 | |
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 B3PW91/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.471 |
|
|
|
2 |
N |
0.180 |
|
|
|
3 |
C |
0.033 |
|
|
|
4 |
H |
0.258 |
|
|
|
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 |
3.094 |
3.094 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.390 |
0.000 |
0.000 |
y |
0.000 |
-16.390 |
0.000 |
z |
0.000 |
0.000 |
-13.453 |
|
Traceless |
| x | y | z |
x |
-1.469 |
0.000 |
0.000 |
y |
0.000 |
-1.469 |
0.000 |
z |
0.000 |
0.000 |
2.937 |
|
Polar |
3z2-r2 | 5.874 |
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 |
1.352 |
0.000 |
0.000 |
y |
0.000 |
1.352 |
0.000 |
z |
0.000 |
0.000 |
5.459 |
<r2> (average value of r
2) Å
2
<r2> |
34.265 |
(<r2>)1/2 |
5.854 |