Jump to
S1C2
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -168.478711 |
| Energy at 298.15K | |
| HF Energy | -168.299241 |
| Nuclear repulsion energy | 60.334356 |
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 B2PLYP/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 |
3530 |
3530 |
258.80 |
28.40 |
0.26 |
0.41 |
| 2 |
Σ |
2294 |
2294 |
376.24 |
14.32 |
0.08 |
0.15 |
| 3 |
Σ |
1295 |
1295 |
83.27 |
26.39 |
0.29 |
0.45 |
| 4 |
Π |
560 |
560 |
1.45 |
0.21 |
0.75 |
0.86 |
| 4 |
Π |
560 |
560 |
1.45 |
0.21 |
0.75 |
0.86 |
| 5 |
Π |
122i |
122i |
86.86 |
4.57 |
0.75 |
0.86 |
| 5 |
Π |
122i |
122i |
86.86 |
4.57 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 3997.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3997.2 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 B2PLYP/6-311G**
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 |
-0.017 |
| C3 |
0.000 |
0.000 |
-1.185 |
| H4 |
0.000 |
0.000 |
-2.244 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.2002 | 2.3685 | 3.4276 |
N2 | 1.2002 | | 1.1683 | 2.2274 | C3 | 2.3685 | 1.1683 | | 1.0591 | H4 | 3.4276 | 2.2274 | 1.0591 | |
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 B2PLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.330 |
|
|
|
| 2 |
N |
0.084 |
|
|
|
| 3 |
C |
0.042 |
|
|
|
| 4 |
H |
0.204 |
|
|
|
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 |
-2.974 |
2.974 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.714 |
0.000 |
0.000 |
| y |
0.000 |
-16.714 |
0.000 |
| z |
0.000 |
0.000 |
-14.066 |
|
| Traceless |
| | x | y | z |
| x |
-1.324 |
0.000 |
0.000 |
| y |
0.000 |
-1.324 |
0.000 |
| z |
0.000 |
0.000 |
2.647 |
|
| Polar |
| 3z2-r2 | 5.295 |
| 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 |
1.458 |
0.000 |
0.000 |
| y |
0.000 |
1.458 |
0.000 |
| z |
0.000 |
0.000 |
5.800 |
<r2> (average value of r
2) Å
2
| <r2> |
34.552 |
| (<r2>)1/2 |
5.878 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -168.478740 |
| Energy at 298.15K | -168.479263 |
| HF Energy | -168.298282 |
| Nuclear repulsion energy | 60.323189 |
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 B2PLYP/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' |
3510 |
3510 |
226.37 |
|
|
|
| 2 |
A' |
2280 |
2280 |
384.81 |
|
|
|
| 3 |
A' |
1298 |
1298 |
73.04 |
|
|
|
| 4 |
A' |
559 |
559 |
2.44 |
|
|
|
| 5 |
A' |
219 |
219 |
123.96 |
|
|
|
| 6 |
A" |
560 |
560 |
1.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4212.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4212.8 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 B2PLYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.757 |
-0.908 |
0.000 |
| N2 |
0.000 |
0.022 |
0.000 |
| C3 |
0.798 |
0.880 |
0.000 |
| H4 |
1.269 |
1.830 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1986 | 2.3693 | 3.4060 |
N2 | 1.1986 | | 1.1719 | 2.2094 | C3 | 2.3693 | 1.1719 | | 1.0605 | H4 | 3.4060 | 2.2094 | 1.0605 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
176.268 |
|
N2 |
C3 |
H4 |
163.527 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.323 |
|
|
|
| 2 |
N |
0.106 |
|
|
|
| 3 |
C |
0.018 |
|
|
|
| 4 |
H |
0.199 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.542 |
2.403 |
0.000 |
2.855 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.431 |
1.035 |
0.000 |
| y |
1.035 |
-14.518 |
0.000 |
| z |
0.000 |
0.000 |
-16.727 |
|
| Traceless |
| | x | y | z |
| x |
-0.808 |
1.035 |
0.000 |
| y |
1.035 |
2.061 |
0.000 |
| z |
0.000 |
0.000 |
-1.252 |
|
| Polar |
| 3z2-r2 | -2.505 |
| x2-y2 | -1.913 |
| xy | 1.035 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.404 |
2.158 |
0.000 |
| y |
2.158 |
3.911 |
0.000 |
| z |
0.000 |
0.000 |
1.460 |
<r2> (average value of r
2) Å
2
| <r2> |
34.531 |
| (<r2>)1/2 |
5.876 |