Jump to
S1C2
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -150.646116 |
| Energy at 298.15K | -150.647969 |
| HF Energy | -150.646116 |
| Nuclear repulsion energy | 35.403092 |
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 B3PW91/3-21G*
| 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 |
3479 |
3338 |
0.00 |
|
|
|
| 2 |
A |
1504 |
1443 |
0.00 |
|
|
|
| 3 |
A |
1017 |
975 |
0.00 |
|
|
|
| 4 |
A |
67 |
64 |
362.03 |
|
|
|
| 5 |
B |
3504 |
3362 |
19.04 |
|
|
|
| 6 |
B |
1177 |
1129 |
151.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5373.2 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 5155.1 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 B3PW91/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.760 |
-0.000 |
| O2 |
0.000 |
-0.760 |
-0.000 |
| H3 |
0.991 |
0.875 |
0.000 |
| H4 |
-0.991 |
-0.875 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.5197 | 0.9975 | 1.9115 |
O2 | 1.5197 | | 1.9115 | 0.9975 | H3 | 0.9975 | 1.9115 | | 2.6435 | H4 | 1.9115 | 0.9975 | 2.6435 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
96.613 |
|
O2 |
O1 |
H3 |
96.613 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.381 |
|
|
|
| 2 |
O |
-0.381 |
|
|
|
| 3 |
H |
0.381 |
|
|
|
| 4 |
H |
0.381 |
|
|
|
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 |
0.002 |
0.002 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.553 |
3.638 |
0.000 |
| y |
3.638 |
-11.008 |
0.000 |
| z |
0.000 |
0.000 |
-12.118 |
|
| Traceless |
| | x | y | z |
| x |
4.010 |
3.638 |
0.000 |
| y |
3.638 |
-1.173 |
0.000 |
| z |
0.000 |
0.000 |
-2.838 |
|
| Polar |
| 3z2-r2 | -5.675 |
| x2-y2 | 3.455 |
| xy | 3.638 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.548 |
0.449 |
0.000 |
| y |
0.449 |
1.908 |
0.000 |
| z |
0.000 |
0.000 |
0.190 |
<r2> (average value of r
2) Å
2
| <r2> |
19.119 |
| (<r2>)1/2 |
4.373 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -150.646116 |
| Energy at 298.15K | -150.647957 |
| HF Energy | -150.646116 |
| Nuclear repulsion energy | 35.403195 |
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 B3PW91/3-21G*
| 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 |
3480 |
3338 |
0.00 |
|
|
|
| 2 |
Ag |
1504 |
1443 |
0.00 |
|
|
|
| 3 |
Ag |
1016 |
975 |
0.00 |
|
|
|
| 4 |
Au |
61 |
58 |
362.07 |
|
|
|
| 5 |
Bu |
3505 |
3363 |
19.05 |
|
|
|
| 6 |
Bu |
1176 |
1129 |
151.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5370.6 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 5152.5 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 B3PW91/3-21G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.760 |
0.000 |
| O2 |
0.000 |
-0.760 |
0.000 |
| H3 |
0.991 |
0.875 |
0.000 |
| H4 |
-0.991 |
-0.875 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.5198 | 0.9974 | 1.9114 |
O2 | 1.5198 | | 1.9114 | 0.9974 | H3 | 0.9974 | 1.9114 | | 2.6433 | H4 | 1.9114 | 0.9974 | 2.6433 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
96.610 |
|
O2 |
O1 |
H3 |
96.610 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.381 |
|
|
|
| 2 |
O |
-0.381 |
|
|
|
| 3 |
H |
0.381 |
|
|
|
| 4 |
H |
0.381 |
|
|
|
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 |
-7.553 |
3.638 |
0.000 |
| y |
3.638 |
-11.008 |
0.000 |
| z |
0.000 |
0.000 |
-12.118 |
|
| Traceless |
| | x | y | z |
| x |
4.010 |
3.638 |
0.000 |
| y |
3.638 |
-1.173 |
0.000 |
| z |
0.000 |
0.000 |
-2.837 |
|
| Polar |
| 3z2-r2 | -5.674 |
| x2-y2 | 3.455 |
| xy | 3.638 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.547 |
0.449 |
0.000 |
| y |
0.449 |
1.908 |
0.000 |
| z |
0.000 |
0.000 |
0.190 |
<r2> (average value of r
2) Å
2
| <r2> |
19.119 |
| (<r2>)1/2 |
4.373 |