Jump to
S1C2
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -168.521119 |
| Energy at 298.15K | |
| HF Energy | -168.521119 |
| Nuclear repulsion energy | 60.444617 |
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/cc-pVDZ
| 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 |
3534 |
3411 |
266.60 |
|
|
|
| 2 |
Σ |
2369 |
2286 |
349.39 |
|
|
|
| 3 |
Σ |
1340 |
1293 |
106.90 |
|
|
|
| 4 |
Xpi |
577 |
557 |
0.49 |
|
|
|
| 4 |
Xpi |
577 |
557 |
0.49 |
|
|
|
| 5 |
Xpi |
84 |
81 |
87.82 |
|
|
|
| 5 |
Xpi |
84 |
81 |
87.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4282.7 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 4132.8 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 B3PW91/cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.181 |
| N2 |
0.000 |
0.000 |
-0.015 |
| C3 |
0.000 |
0.000 |
-1.182 |
| H4 |
0.000 |
0.000 |
-2.251 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1955 | 2.3624 | 3.4318 |
N2 | 1.1955 | | 1.1669 | 2.2363 | C3 | 2.3624 | 1.1669 | | 1.0694 | H4 | 3.4318 | 2.2363 | 1.0694 | |
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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.288 |
|
|
|
| 2 |
N |
0.206 |
|
|
|
| 3 |
C |
-0.042 |
|
|
|
| 4 |
H |
0.124 |
|
|
|
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 |
-2.905 |
2.905 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.455 |
0.000 |
0.000 |
| y |
0.000 |
-16.455 |
0.000 |
| z |
0.000 |
0.000 |
-13.702 |
|
| Traceless |
| | x | y | z |
| x |
-1.376 |
0.000 |
0.000 |
| y |
0.000 |
-1.376 |
0.000 |
| z |
0.000 |
0.000 |
2.753 |
|
| Polar |
| 3z2-r2 | 5.506 |
| 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 |
1.402 |
0.000 |
0.000 |
| y |
0.000 |
1.402 |
0.000 |
| z |
0.000 |
0.000 |
5.557 |
<r2> (average value of r
2) Å
2
| <r2> |
34.305 |
| (<r2>)1/2 |
5.857 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -168.521120 |
| Energy at 298.15K | -168.521469 |
| HF Energy | -168.521120 |
| Nuclear repulsion energy | 60.446583 |
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/cc-pVDZ
| 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' |
3533 |
3409 |
266.70 |
|
|
|
| 2 |
A' |
2369 |
2287 |
349.74 |
|
|
|
| 3 |
A' |
1341 |
1294 |
106.71 |
|
|
|
| 4 |
A' |
577 |
557 |
0.52 |
|
|
|
| 5 |
A' |
95 |
92 |
87.83 |
|
|
|
| 6 |
A" |
577 |
557 |
0.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4246.1 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 4097.5 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/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.010 |
-1.181 |
0.000 |
| N2 |
0.000 |
0.015 |
0.000 |
| C3 |
0.011 |
1.182 |
0.000 |
| H4 |
0.018 |
2.251 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1954 | 2.3623 | 3.4320 |
N2 | 1.1954 | | 1.1670 | 2.2366 | C3 | 2.3623 | 1.1670 | | 1.0696 | H4 | 3.4320 | 2.2366 | 1.0696 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.964 |
|
N2 |
C3 |
H4 |
179.845 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.288 |
|
|
|
| 2 |
N |
0.206 |
|
|
|
| 3 |
C |
-0.042 |
|
|
|
| 4 |
H |
0.124 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.022 |
2.904 |
0.000 |
2.904 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.455 |
0.017 |
0.000 |
| y |
0.017 |
-13.701 |
0.000 |
| z |
0.000 |
0.000 |
-16.455 |
|
| Traceless |
| | x | y | z |
| x |
-1.377 |
0.017 |
0.000 |
| y |
0.017 |
2.754 |
0.000 |
| z |
0.000 |
0.000 |
-1.377 |
|
| Polar |
| 3z2-r2 | -2.754 |
| x2-y2 | -2.754 |
| 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 |
1.402 |
0.038 |
0.000 |
| y |
0.038 |
5.557 |
0.000 |
| z |
0.000 |
0.000 |
1.402 |
<r2> (average value of r
2) Å
2
| <r2> |
34.304 |
| (<r2>)1/2 |
5.857 |