Jump to
S1C2
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -168.520520 |
| Energy at 298.15K | |
| HF Energy | -168.520520 |
| Nuclear repulsion energy | 60.662580 |
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(2df,p)
| 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 |
3530 |
3394 |
251.92 |
24.82 |
0.24 |
0.39 |
| 2 |
Σ |
2378 |
2286 |
325.94 |
20.59 |
0.17 |
0.30 |
| 3 |
Σ |
1334 |
1282 |
105.13 |
20.37 |
0.24 |
0.38 |
| 4 |
Π |
585 |
563 |
0.91 |
0.77 |
0.75 |
0.86 |
| 4 |
Π |
585 |
563 |
0.91 |
0.77 |
0.75 |
0.86 |
| 5 |
Π |
125 |
120 |
75.04 |
1.55 |
0.75 |
0.86 |
| 5 |
Π |
125 |
120 |
75.04 |
1.55 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4330.7 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 4163.5 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(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.178 |
| N2 |
0.000 |
0.000 |
-0.018 |
| C3 |
0.000 |
0.000 |
-1.177 |
| H4 |
0.000 |
0.000 |
-2.238 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1950 | 2.3542 | 3.4151 |
N2 | 1.1950 | | 1.1591 | 2.2200 | C3 | 2.3542 | 1.1591 | | 1.0609 | H4 | 3.4151 | 2.2200 | 1.0609 | |
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(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.455 |
|
|
|
| 2 |
N |
0.446 |
|
|
|
| 3 |
C |
-0.268 |
|
|
|
| 4 |
H |
0.277 |
|
|
|
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 |
-2.997 |
2.997 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.382 |
0.000 |
0.000 |
| y |
0.000 |
-16.382 |
0.000 |
| z |
0.000 |
0.000 |
-13.271 |
|
| Traceless |
| | x | y | z |
| x |
-1.556 |
0.000 |
0.000 |
| y |
0.000 |
-1.556 |
0.000 |
| z |
0.000 |
0.000 |
3.111 |
|
| Polar |
| 3z2-r2 | 6.222 |
| 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 |
1.731 |
0.000 |
0.000 |
| y |
0.000 |
1.731 |
0.000 |
| z |
0.000 |
0.000 |
5.442 |
<r2> (average value of r
2) Å
2
| <r2> |
33.992 |
| (<r2>)1/2 |
5.830 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -168.520521 |
| Energy at 298.15K | -168.520927 |
| HF Energy | -168.520521 |
| Nuclear repulsion energy | 60.657769 |
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(2df,p)
| 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' |
3530 |
3394 |
251.82 |
|
|
|
| 2 |
A' |
2378 |
2286 |
326.02 |
|
|
|
| 3 |
A' |
1334 |
1282 |
105.01 |
|
|
|
| 4 |
A' |
585 |
563 |
0.90 |
|
|
|
| 5 |
A' |
124 |
119 |
75.05 |
|
|
|
| 6 |
A" |
585 |
563 |
1.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4267.9 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 4103.1 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(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.009 |
-1.178 |
0.000 |
| N2 |
0.000 |
0.018 |
0.000 |
| C3 |
0.010 |
1.177 |
0.000 |
| H4 |
0.016 |
2.238 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1951 | 2.3544 | 3.4153 |
N2 | 1.1951 | | 1.1593 | 2.2202 | C3 | 2.3544 | 1.1593 | | 1.0610 | H4 | 3.4153 | 2.2202 | 1.0610 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.961 |
|
N2 |
C3 |
H4 |
179.825 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.455 |
|
|
|
| 2 |
N |
0.446 |
|
|
|
| 3 |
C |
-0.268 |
|
|
|
| 4 |
H |
0.277 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.021 |
2.997 |
0.000 |
2.997 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.382 |
0.017 |
0.000 |
| y |
0.017 |
-13.270 |
0.000 |
| z |
0.000 |
0.000 |
-16.382 |
|
| Traceless |
| | x | y | z |
| x |
-1.556 |
0.017 |
0.000 |
| y |
0.017 |
3.113 |
0.000 |
| z |
0.000 |
0.000 |
-1.556 |
|
| Polar |
| 3z2-r2 | -3.113 |
| x2-y2 | -3.112 |
| 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 |
1.731 |
0.031 |
0.000 |
| y |
0.031 |
5.443 |
0.000 |
| z |
0.000 |
0.000 |
1.731 |
<r2> (average value of r
2) Å
2
| <r2> |
33.996 |
| (<r2>)1/2 |
5.831 |