Jump to
S1C2
Energy calculated at B3PW91/6-31G
| | hartrees |
| Energy at 0K | -168.443084 |
| Energy at 298.15K | |
| HF Energy | -168.443084 |
| Nuclear repulsion energy | 59.422409 |
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 |
3570 |
3419 |
230.90 |
|
|
|
| 2 |
Σ |
2296 |
2199 |
214.84 |
|
|
|
| 3 |
Σ |
1212 |
1160 |
90.85 |
|
|
|
| 4 |
Xpi |
514 |
492 |
4.31 |
|
|
|
| 4 |
Xpi |
514 |
492 |
4.31 |
|
|
|
| 5 |
Xpi |
371 |
355 |
111.68 |
|
|
|
| 5 |
Xpi |
371 |
355 |
111.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4423.2 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 4236.1 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 |
1.207 |
| N2 |
0.000 |
0.000 |
-0.029 |
| C3 |
0.000 |
0.000 |
-1.199 |
| H4 |
0.000 |
0.000 |
-2.259 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.2353 | 2.4052 | 3.4659 |
N2 | 1.2353 | | 1.1700 | 2.2307 | C3 | 2.4052 | 1.1700 | | 1.0607 | H4 | 3.4659 | 2.2307 | 1.0607 | |
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 |
-0.379 |
|
|
|
| 2 |
N |
0.062 |
|
|
|
| 3 |
C |
0.006 |
|
|
|
| 4 |
H |
0.310 |
|
|
|
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 |
-3.543 |
3.543 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.601 |
0.000 |
0.000 |
| y |
0.000 |
-16.601 |
0.000 |
| z |
0.000 |
0.000 |
-14.233 |
|
| Traceless |
| | x | y | z |
| x |
-1.184 |
0.000 |
0.000 |
| y |
0.000 |
-1.184 |
0.000 |
| z |
0.000 |
0.000 |
2.368 |
|
| Polar |
| 3z2-r2 | 4.736 |
| 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 |
1.091 |
0.000 |
0.000 |
| y |
0.000 |
1.091 |
0.000 |
| z |
0.000 |
0.000 |
5.626 |
<r2> (average value of r
2) Å
2
| <r2> |
35.253 |
| (<r2>)1/2 |
5.937 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G
| | hartrees |
| Energy at 0K | -168.443085 |
| Energy at 298.15K | -168.443703 |
| HF Energy | -168.443085 |
| Nuclear repulsion energy | 59.415732 |
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 |
A' |
3571 |
3420 |
230.82 |
|
|
|
| 2 |
A' |
2296 |
2199 |
214.30 |
|
|
|
| 3 |
A' |
1210 |
1159 |
90.96 |
|
|
|
| 4 |
A' |
514 |
492 |
4.18 |
|
|
|
| 5 |
A' |
370 |
354 |
111.74 |
|
|
|
| 6 |
A" |
498 |
477 |
32.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4229.2 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 4050.3 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 B3PW91/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.008 |
-1.207 |
0.000 |
| N2 |
0.000 |
0.029 |
0.000 |
| C3 |
0.008 |
1.199 |
0.000 |
| H4 |
0.015 |
2.259 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.2356 | 2.4055 | 3.4662 |
N2 | 1.2356 | | 1.1699 | 2.2306 | C3 | 2.4055 | 1.1699 | | 1.0606 | H4 | 3.4662 | 2.2306 | 1.0606 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.966 |
|
N2 |
C3 |
H4 |
179.925 |
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 |
-0.379 |
|
|
|
| 2 |
N |
0.062 |
|
|
|
| 3 |
C |
0.007 |
|
|
|
| 4 |
H |
0.310 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.022 |
3.545 |
0.000 |
3.545 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.601 |
0.013 |
0.000 |
| y |
0.013 |
-14.231 |
0.000 |
| z |
0.000 |
0.000 |
-16.601 |
|
| Traceless |
| | x | y | z |
| x |
-1.185 |
0.013 |
0.000 |
| y |
0.013 |
2.370 |
0.000 |
| z |
0.000 |
0.000 |
-1.185 |
|
| Polar |
| 3z2-r2 | -2.370 |
| x2-y2 | -2.370 |
| xy | 0.013 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.091 |
0.031 |
0.000 |
| y |
0.031 |
5.627 |
0.000 |
| z |
0.000 |
0.000 |
1.091 |
<r2> (average value of r
2) Å
2
| <r2> |
35.258 |
| (<r2>)1/2 |
5.938 |