Jump to
S1C2
Energy calculated at HF/cc-pVDZ
| hartrees |
Energy at 0K | -258.444242 |
Energy at 298.15K | -258.445724 |
HF Energy | -258.444242 |
Nuclear repulsion energy | 108.254174 |
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/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 |
A1 |
2108 |
1914 |
44.18 |
|
|
|
2 |
A1 |
509 |
462 |
0.42 |
|
|
|
3 |
A1 |
436 |
396 |
0.75 |
|
|
|
4 |
A2 |
116 |
106 |
0.00 |
|
|
|
5 |
B2 |
2005 |
1821 |
486.31 |
|
|
|
6 |
B2 |
975 |
885 |
41.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3074.5 cm
-1
Scaled (by 0.908) Zero Point Vibrational Energy (zpe) 2791.7 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/cc-pVDZ
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
0.115 |
|
|
|
2 |
N |
0.115 |
|
|
|
3 |
O |
-0.115 |
|
|
|
4 |
O |
-0.115 |
|
|
|
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 |
0.423 |
0.423 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.827 |
0.000 |
0.000 |
y |
0.000 |
-23.331 |
0.000 |
z |
0.000 |
0.000 |
-22.886 |
|
Traceless |
| x | y | z |
x |
4.281 |
0.000 |
0.000 |
y |
0.000 |
-2.474 |
0.000 |
z |
0.000 |
0.000 |
-1.807 |
|
Polar |
3z2-r2 | -3.614 |
x2-y2 | 4.503 |
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 |
1.404 |
0.000 |
0.000 |
y |
0.000 |
4.246 |
0.000 |
z |
0.000 |
0.000 |
2.825 |
<r2> (average value of r
2) Å
2
<r2> |
54.119 |
(<r2>)1/2 |
7.357 |
Jump to
S1C1
Energy calculated at HF/cc-pVDZ
| hartrees |
Energy at 0K | -258.446079 |
Energy at 298.15K | -258.447551 |
HF Energy | -258.446079 |
Nuclear repulsion energy | 106.701862 |
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/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 |
Ag |
2066 |
1876 |
0.00 |
|
|
|
2 |
Ag |
1044 |
948 |
0.00 |
|
|
|
3 |
Ag |
549 |
498 |
0.00 |
|
|
|
4 |
Au |
64 |
58 |
1.20 |
|
|
|
5 |
Bu |
2015 |
1830 |
325.47 |
|
|
|
6 |
Bu |
489 |
444 |
6.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3112.8 cm
-1
Scaled (by 0.908) Zero Point Vibrational Energy (zpe) 2826.4 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/cc-pVDZ
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
-0.382 |
0.659 |
0.000 |
N2 |
0.382 |
-0.659 |
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 | | 1.5224 | 1.1486 | 2.1756 |
N2 | 1.5224 | | 2.1756 | 1.1486 | O3 | 1.1486 | 2.1756 | | 3.1284 | O4 | 2.1756 | 1.1486 | 3.1284 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
N2 |
O4 |
108.264 |
|
N2 |
N1 |
O3 |
108.264 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
0.128 |
|
|
|
2 |
N |
0.128 |
|
|
|
3 |
O |
-0.128 |
|
|
|
4 |
O |
-0.128 |
|
|
|
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 |
-22.985 |
-0.366 |
0.000 |
y |
-0.366 |
-23.925 |
0.000 |
z |
0.000 |
0.000 |
-18.816 |
|
Traceless |
| x | y | z |
x |
-1.615 |
-0.366 |
0.000 |
y |
-0.366 |
-3.024 |
0.000 |
z |
0.000 |
0.000 |
4.640 |
|
Polar |
3z2-r2 | 9.279 |
x2-y2 | 0.939 |
xy | -0.366 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.181 |
0.742 |
0.000 |
y |
0.742 |
4.735 |
0.000 |
z |
0.000 |
0.000 |
1.419 |
<r2> (average value of r
2) Å
2
<r2> |
60.943 |
(<r2>)1/2 |
7.807 |