Jump to
S1C2
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -151.518926 |
| Energy at 298.15K | -151.521204 |
| HF Energy | -151.518926 |
| Nuclear repulsion energy | 37.064021 |
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 B3PW91/6-311G*
| 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 |
3770 |
3629 |
4.38 |
|
|
|
| 2 |
A |
1514 |
1457 |
0.24 |
|
|
|
| 3 |
A |
978 |
941 |
2.13 |
|
|
|
| 4 |
A |
355 |
341 |
245.22 |
|
|
|
| 5 |
B |
3773 |
3632 |
28.40 |
|
|
|
| 6 |
B |
1350 |
1300 |
105.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5869.5 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 5650.5 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 B3PW91/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.719 |
-0.052 |
| O2 |
0.000 |
-0.719 |
-0.052 |
| H3 |
0.823 |
0.899 |
0.418 |
| H4 |
-0.823 |
-0.899 |
0.418 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4375 | 0.9651 | 1.8754 |
O2 | 1.4375 | | 1.8754 | 0.9651 | H3 | 0.9651 | 1.8754 | | 2.4381 | H4 | 1.8754 | 0.9651 | 2.4381 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
100.781 |
|
O2 |
O1 |
H3 |
100.781 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.419 |
|
|
|
| 2 |
O |
-0.419 |
|
|
|
| 3 |
H |
0.419 |
|
|
|
| 4 |
H |
0.419 |
|
|
|
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 |
1.873 |
1.873 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.167 |
3.291 |
0.000 |
| y |
3.291 |
-11.256 |
0.000 |
| z |
0.000 |
0.000 |
-11.766 |
|
| Traceless |
| | x | y | z |
| x |
2.344 |
3.291 |
0.000 |
| y |
3.291 |
-0.789 |
0.000 |
| z |
0.000 |
0.000 |
-1.555 |
|
| Polar |
| 3z2-r2 | -3.110 |
| x2-y2 | 2.088 |
| xy | 3.291 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.367 |
0.326 |
0.000 |
| y |
0.326 |
2.008 |
0.000 |
| z |
0.000 |
0.000 |
0.914 |
<r2> (average value of r
2) Å
2
| <r2> |
18.333 |
| (<r2>)1/2 |
4.282 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -151.517925 |
| Energy at 298.15K | |
| HF Energy | -151.517925 |
| Nuclear repulsion energy | 36.910206 |
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 B3PW91/6-311G*
| 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 |
3805 |
3663 |
0.00 |
|
|
|
| 2 |
Ag |
1600 |
1540 |
0.00 |
|
|
|
| 3 |
Ag |
977 |
940 |
0.00 |
|
|
|
| 4 |
Au |
254i |
244i |
363.59 |
|
|
|
| 5 |
Bu |
3818 |
3675 |
60.58 |
|
|
|
| 6 |
Bu |
1277 |
1229 |
142.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5611.0 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 5401.7 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 B3PW91/6-311G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.724 |
0.000 |
| O2 |
0.000 |
-0.724 |
0.000 |
| H3 |
0.951 |
0.878 |
0.000 |
| H4 |
-0.951 |
-0.878 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4487 | 0.9637 | 1.8638 |
O2 | 1.4487 | | 1.8638 | 0.9637 | H3 | 0.9637 | 1.8638 | | 2.5897 | H4 | 1.8638 | 0.9637 | 2.5897 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
99.199 |
|
O2 |
O1 |
H3 |
99.199 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.425 |
|
|
|
| 2 |
O |
-0.425 |
|
|
|
| 3 |
H |
0.425 |
|
|
|
| 4 |
H |
0.425 |
|
|
|
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 |
-7.914 |
3.780 |
0.000 |
| y |
3.780 |
-11.389 |
0.000 |
| z |
0.000 |
0.000 |
-12.738 |
|
| Traceless |
| | x | y | z |
| x |
4.149 |
3.780 |
0.000 |
| y |
3.780 |
-1.062 |
0.000 |
| z |
0.000 |
0.000 |
-3.087 |
|
| Polar |
| 3z2-r2 | -6.174 |
| x2-y2 | 3.475 |
| xy | 3.780 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.570 |
0.336 |
0.000 |
| y |
0.336 |
2.023 |
0.000 |
| z |
0.000 |
0.000 |
0.698 |
<r2> (average value of r
2) Å
2
| <r2> |
18.419 |
| (<r2>)1/2 |
4.292 |