Jump to
S1C2
Energy calculated at LSDA/cc-pVDZ
| | hartrees |
| Energy at 0K | -167.706328 |
| Energy at 298.15K | |
| HF Energy | -167.706328 |
| Nuclear repulsion energy | 60.332532 |
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 LSDA/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 |
3460 |
3422 |
269.42 |
|
|
|
| 2 |
Σ |
2361 |
2335 |
294.08 |
|
|
|
| 3 |
Σ |
1353 |
1338 |
70.30 |
|
|
|
| 4 |
Π |
571 |
564 |
0.24 |
|
|
|
| 4 |
Π |
571 |
564 |
0.24 |
|
|
|
| 5 |
Π |
145i |
144i |
88.37 |
|
|
|
| 5 |
Π |
145i |
144i |
88.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4012.3 cm
-1
Scaled (by 0.989) Zero Point Vibrational Energy (zpe) 3968.2 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 LSDA/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 |
-0.010 |
| C3 |
0.000 |
0.000 |
-1.186 |
| H4 |
0.000 |
0.000 |
-2.264 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1908 | 2.3668 | 3.4453 |
N2 | 1.1908 | | 1.1760 | 2.2545 | C3 | 2.3668 | 1.1760 | | 1.0785 | H4 | 3.4453 | 2.2545 | 1.0785 | |
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 LSDA/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.224 |
|
|
|
| 2 |
N |
0.204 |
|
|
|
| 3 |
C |
-0.109 |
|
|
|
| 4 |
H |
0.130 |
|
|
|
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 |
-2.534 |
2.534 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.534 |
0.000 |
0.000 |
| y |
0.000 |
-16.534 |
0.000 |
| z |
0.000 |
0.000 |
-13.750 |
|
| Traceless |
| | x | y | z |
| x |
-1.392 |
0.000 |
0.000 |
| y |
0.000 |
-1.392 |
0.000 |
| z |
0.000 |
0.000 |
2.784 |
|
| Polar |
| 3z2-r2 | 5.568 |
| 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 |
1.420 |
0.000 |
0.000 |
| y |
0.000 |
1.420 |
0.000 |
| z |
0.000 |
0.000 |
5.593 |
<r2> (average value of r
2) Å
2
| <r2> |
34.470 |
| (<r2>)1/2 |
5.871 |
Jump to
S1C1
Energy calculated at LSDA/cc-pVDZ
| | hartrees |
| Energy at 0K | -167.706377 |
| Energy at 298.15K | -167.706901 |
| HF Energy | -167.706377 |
| Nuclear repulsion energy | 60.327449 |
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 LSDA/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' |
3435 |
3397 |
240.53 |
|
|
|
| 2 |
A' |
2350 |
2324 |
304.33 |
|
|
|
| 3 |
A' |
1355 |
1340 |
63.30 |
|
|
|
| 4 |
A' |
569 |
562 |
0.73 |
|
|
|
| 5 |
A' |
208 |
206 |
111.57 |
|
|
|
| 6 |
A" |
570 |
564 |
0.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4243.3 cm
-1
Scaled (by 0.989) Zero Point Vibrational Energy (zpe) 4196.6 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 LSDA/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.878 |
-0.787 |
0.000 |
| N2 |
0.000 |
0.015 |
0.000 |
| C3 |
0.916 |
0.757 |
0.000 |
| H4 |
1.526 |
1.649 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1896 | 2.3673 | 3.4226 |
N2 | 1.1896 | | 1.1788 | 2.2353 | C3 | 2.3673 | 1.1788 | | 1.0803 | H4 | 3.4226 | 2.2353 | 1.0803 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
176.548 |
|
N2 |
C3 |
H4 |
163.352 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.220 |
|
|
|
| 2 |
N |
0.210 |
|
|
|
| 3 |
C |
-0.122 |
|
|
|
| 4 |
H |
0.131 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.549 |
1.886 |
0.000 |
2.441 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.884 |
1.316 |
0.000 |
| y |
1.316 |
-14.594 |
0.000 |
| z |
0.000 |
0.000 |
-16.548 |
|
| Traceless |
| | x | y | z |
| x |
-0.313 |
1.316 |
0.000 |
| y |
1.316 |
1.621 |
0.000 |
| z |
0.000 |
0.000 |
-1.309 |
|
| Polar |
| 3z2-r2 | -2.618 |
| x2-y2 | -1.289 |
| xy | 1.316 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.846 |
2.057 |
0.000 |
| y |
2.057 |
3.220 |
0.000 |
| z |
0.000 |
0.000 |
1.420 |
<r2> (average value of r
2) Å
2
| <r2> |
34.441 |
| (<r2>)1/2 |
5.869 |