Jump to
S1C2
Energy calculated at HF/6-31G*
| hartrees |
Energy at 0K | -258.416569 |
Energy at 298.15K | |
HF Energy | -258.416569 |
Nuclear repulsion energy | 108.287251 |
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 HF/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 |
A1 |
2085 |
1874 |
37.31 |
|
|
|
2 |
A1 |
561 |
504 |
1.02 |
|
|
|
3 |
A1 |
442 |
397 |
0.95 |
|
|
|
4 |
A2 |
42i |
37i |
0.00 |
|
|
|
5 |
B2 |
2011 |
1807 |
369.26 |
|
|
|
6 |
B2 |
978 |
879 |
46.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3018.1 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 2711.7 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 HF/6-31G*
Point Group is C2v
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
0.194 |
|
|
|
2 |
N |
0.194 |
|
|
|
3 |
O |
-0.194 |
|
|
|
4 |
O |
-0.194 |
|
|
|
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 |
0.386 |
0.386 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.000 |
0.000 |
0.000 |
y |
0.000 |
-23.453 |
0.000 |
z |
0.000 |
0.000 |
-22.915 |
|
Traceless |
| x | y | z |
x |
4.184 |
0.000 |
0.000 |
y |
0.000 |
-2.495 |
0.000 |
z |
0.000 |
0.000 |
-1.689 |
|
Polar |
3z2-r2 | -3.377 |
x2-y2 | 4.453 |
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 |
1.575 |
0.000 |
0.000 |
y |
0.000 |
4.164 |
0.000 |
z |
0.000 |
0.000 |
2.894 |
<r2> (average value of r
2) Å
2
<r2> |
53.969 |
(<r2>)1/2 |
7.346 |
Jump to
S1C1
Energy calculated at HF/6-31G*
| hartrees |
Energy at 0K | -258.419698 |
Energy at 298.15K | -258.421117 |
HF Energy | -258.419698 |
Nuclear repulsion energy | 106.665582 |
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 HF/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 |
Ag |
2055 |
1846 |
0.00 |
|
|
|
2 |
Ag |
1060 |
952 |
0.00 |
|
|
|
3 |
Ag |
580 |
521 |
0.00 |
|
|
|
4 |
Au |
27 |
25 |
1.18 |
|
|
|
5 |
Bu |
2015 |
1810 |
279.96 |
|
|
|
6 |
Bu |
498 |
447 |
6.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3116.8 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 2800.4 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 HF/6-31G*
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
-0.382 |
0.650 |
0.000 |
N2 |
0.382 |
-0.650 |
0.000 |
O3 |
0.382 |
1.517 |
0.000 |
O4 |
-0.382 |
-1.517 |
0.000 |
Atom - Atom Distances (Å)
|
N1 |
N2 |
O3 |
O4 |
N1 | | 1.5076 | 1.1553 | 2.1676 |
N2 | 1.5076 | | 2.1676 | 1.1553 | O3 | 1.1553 | 2.1676 | | 3.1294 | O4 | 2.1676 | 1.1553 | 3.1294 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
N2 |
O4 |
108.249 |
|
N2 |
N1 |
O3 |
108.249 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
0.210 |
|
|
|
2 |
N |
0.210 |
|
|
|
3 |
O |
-0.210 |
|
|
|
4 |
O |
-0.210 |
|
|
|
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 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.106 |
-0.263 |
0.000 |
y |
-0.263 |
-23.857 |
0.000 |
z |
0.000 |
0.000 |
-18.987 |
|
Traceless |
| x | y | z |
x |
-1.683 |
-0.263 |
0.000 |
y |
-0.263 |
-2.811 |
0.000 |
z |
0.000 |
0.000 |
4.494 |
|
Polar |
3z2-r2 | 8.988 |
x2-y2 | 0.751 |
xy | -0.263 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.284 |
0.731 |
0.000 |
y |
0.731 |
4.775 |
0.000 |
z |
0.000 |
0.000 |
1.585 |
<r2> (average value of r
2) Å
2
<r2> |
60.859 |
(<r2>)1/2 |
7.801 |