Jump to
S1C2
Energy calculated at wB97X-D/LANL2DZ
| | hartrees |
| Energy at 0K | -131.040107 |
| Energy at 298.15K | -131.042533 |
| HF Energy | -131.040107 |
| Nuclear repulsion energy | 34.283170 |
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 wB97X-D/LANL2DZ
| 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 |
3563 |
3563 |
5.40 |
|
|
|
| 2 |
A1 |
1711 |
1711 |
24.51 |
|
|
|
| 3 |
A1 |
1343 |
1343 |
0.00 |
|
|
|
| 4 |
B1 |
474 |
474 |
361.78 |
|
|
|
| 5 |
B2 |
3728 |
3728 |
2.47 |
|
|
|
| 6 |
B2 |
1258 |
1258 |
6.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6037.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6037.5 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 wB97X-D/LANL2DZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.562 |
| O2 |
0.000 |
0.000 |
0.757 |
| H3 |
0.000 |
0.881 |
-1.062 |
| H4 |
0.000 |
-0.881 |
-1.062 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.3183 | 1.0130 | 1.0130 |
O2 | 1.3183 | | 2.0206 | 2.0206 | H3 | 1.0130 | 2.0206 | | 1.7617 | H4 | 1.0130 | 2.0206 | 1.7617 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
119.595 |
|
O2 |
N1 |
H4 |
119.595 |
| H3 |
N1 |
H4 |
120.810 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.418 |
|
|
|
| 2 |
O |
-0.238 |
|
|
|
| 3 |
H |
0.328 |
|
|
|
| 4 |
H |
0.328 |
|
|
|
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 |
-3.331 |
3.331 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.526 |
0.000 |
0.000 |
| y |
0.000 |
-9.813 |
0.000 |
| z |
0.000 |
0.000 |
-10.936 |
|
| Traceless |
| | x | y | z |
| x |
-2.152 |
0.000 |
0.000 |
| y |
0.000 |
1.918 |
0.000 |
| z |
0.000 |
0.000 |
0.233 |
|
| Polar |
| 3z2-r2 | 0.467 |
| x2-y2 | -2.713 |
| 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 |
0.638 |
0.000 |
0.000 |
| y |
0.000 |
1.318 |
0.000 |
| z |
0.000 |
0.000 |
2.879 |
<r2> (average value of r
2) Å
2
| <r2> |
17.523 |
| (<r2>)1/2 |
4.186 |
Jump to
S1C1
Energy calculated at wB97X-D/LANL2DZ
| | hartrees |
| Energy at 0K | -131.040107 |
| Energy at 298.15K | -131.042533 |
| HF Energy | -131.040107 |
| Nuclear repulsion energy | 34.283521 |
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 wB97X-D/LANL2DZ
| 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' |
3563 |
3563 |
5.40 |
|
|
|
| 2 |
A' |
1711 |
1711 |
24.52 |
|
|
|
| 3 |
A' |
1343 |
1343 |
0.00 |
|
|
|
| 4 |
A' |
473 |
473 |
361.84 |
|
|
|
| 5 |
A" |
3728 |
3728 |
2.48 |
|
|
|
| 6 |
A" |
1258 |
1258 |
6.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6037.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6037.6 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 wB97X-D/LANL2DZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.418 |
|
|
|
| 2 |
O |
-0.238 |
|
|
|
| 3 |
H |
0.328 |
|
|
|
| 4 |
H |
0.328 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.002 |
3.331 |
0.000 |
3.331 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.526 |
0.002 |
0.000 |
| y |
0.002 |
-10.936 |
0.000 |
| z |
0.000 |
0.000 |
-9.812 |
|
| Traceless |
| | x | y | z |
| x |
-2.152 |
0.002 |
0.000 |
| y |
0.002 |
0.233 |
0.000 |
| z |
0.000 |
0.000 |
1.919 |
|
| Polar |
| 3z2-r2 | 3.838 |
| x2-y2 | -1.590 |
| xy | 0.002 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.638 |
0.000 |
0.000 |
| y |
0.000 |
2.879 |
0.000 |
| z |
0.000 |
0.000 |
1.318 |
<r2> (average value of r
2) Å
2
| <r2> |
17.522 |
| (<r2>)1/2 |
4.186 |