Jump to
S1C2
Energy calculated at mPW1PW91/STO-3G
| | hartrees |
| Energy at 0K | -129.289819 |
| Energy at 298.15K | |
| HF Energy | -129.289819 |
| Nuclear repulsion energy | 33.516189 |
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 mPW1PW91/STO-3G
| 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 |
3131 |
3.92 |
|
|
|
| 2 |
A1 |
1776 |
1561 |
13.79 |
|
|
|
| 3 |
A1 |
1416 |
1245 |
4.42 |
|
|
|
| 4 |
B1 |
566i |
497i |
257.76 |
|
|
|
| 5 |
B2 |
3771 |
3314 |
3.83 |
|
|
|
| 6 |
B2 |
1204 |
1058 |
0.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5581.8 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 4905.9 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 mPW1PW91/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.566 |
| O2 |
0.000 |
0.000 |
0.775 |
| H3 |
0.000 |
0.888 |
-1.121 |
| H4 |
0.000 |
-0.888 |
-1.121 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.3407 | 1.0476 | 1.0476 |
O2 | 1.3407 | | 2.0941 | 2.0941 | H3 | 1.0476 | 2.0941 | | 1.7761 | H4 | 1.0476 | 2.0941 | 1.7761 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
122.038 |
|
O2 |
N1 |
H4 |
122.038 |
| H3 |
N1 |
H4 |
115.925 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.282 |
|
|
|
| 2 |
O |
-0.105 |
|
|
|
| 3 |
H |
0.194 |
|
|
|
| 4 |
H |
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 |
-2.084 |
2.084 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.858 |
0.000 |
0.000 |
| y |
0.000 |
-9.043 |
0.000 |
| z |
0.000 |
0.000 |
-9.374 |
|
| Traceless |
| | x | y | z |
| x |
-1.649 |
0.000 |
0.000 |
| y |
0.000 |
1.073 |
0.000 |
| z |
0.000 |
0.000 |
0.576 |
|
| Polar |
| 3z2-r2 | 1.151 |
| x2-y2 | -1.815 |
| 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 |
0.243 |
0.000 |
0.000 |
| y |
0.000 |
0.870 |
0.000 |
| z |
0.000 |
0.000 |
1.596 |
<r2> (average value of r
2) Å
2
| <r2> |
17.233 |
| (<r2>)1/2 |
4.151 |
Jump to
S1C1
Energy calculated at mPW1PW91/STO-3G
| | hartrees |
| Energy at 0K | -129.293021 |
| Energy at 298.15K | -129.295537 |
| HF Energy | -129.293021 |
| Nuclear repulsion energy | 33.173593 |
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 mPW1PW91/STO-3G
| 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' |
3449 |
3032 |
1.46 |
|
|
|
| 2 |
A' |
1806 |
1587 |
10.53 |
|
|
|
| 3 |
A' |
1351 |
1187 |
1.18 |
|
|
|
| 4 |
A' |
697 |
613 |
183.06 |
|
|
|
| 5 |
A" |
3653 |
3211 |
14.96 |
|
|
|
| 6 |
A" |
1304 |
1146 |
0.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6130.3 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 5388.0 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 mPW1PW91/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.051 |
0.590 |
0.000 |
| O2 |
-0.051 |
-0.773 |
0.000 |
| H3 |
0.383 |
1.028 |
0.863 |
| H4 |
0.383 |
1.028 |
-0.863 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.3631 | 1.0606 | 1.0606 |
O2 | 1.3631 | | 2.0440 | 2.0440 | H3 | 1.0606 | 2.0440 | | 1.7260 | H4 | 1.0606 | 2.0440 | 1.7260 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
114.409 |
|
O2 |
N1 |
H4 |
114.409 |
| H3 |
N1 |
H4 |
108.920 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.268 |
|
|
|
| 2 |
O |
-0.096 |
|
|
|
| 3 |
H |
0.182 |
|
|
|
| 4 |
H |
0.182 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.307 |
1.574 |
0.000 |
2.046 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.465 |
1.205 |
0.000 |
| y |
1.205 |
-10.185 |
0.000 |
| z |
0.000 |
0.000 |
-9.345 |
|
| Traceless |
| | x | y | z |
| x |
-0.700 |
1.205 |
0.000 |
| y |
1.205 |
-0.280 |
0.000 |
| z |
0.000 |
0.000 |
0.980 |
|
| Polar |
| 3z2-r2 | 1.960 |
| x2-y2 | -0.281 |
| xy | 1.205 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.359 |
0.183 |
0.000 |
| y |
0.183 |
1.553 |
0.000 |
| z |
0.000 |
0.000 |
0.897 |
<r2> (average value of r
2) Å
2
| <r2> |
17.400 |
| (<r2>)1/2 |
4.171 |