Jump to
S1C2
Energy calculated at B3PW91/cc-pVTZ
| | hartrees |
| Energy at 0K | -151.551904 |
| Energy at 298.15K | -151.554217 |
| HF Energy | -151.551904 |
| Nuclear repulsion energy | 37.090159 |
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/cc-pVTZ
| 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 |
3796 |
3650 |
12.88 |
|
|
|
| 2 |
A |
1449 |
1394 |
0.43 |
|
|
|
| 3 |
A |
983 |
946 |
0.99 |
|
|
|
| 4 |
A |
385 |
370 |
167.93 |
|
|
|
| 5 |
B |
3795 |
3649 |
47.69 |
|
|
|
| 6 |
B |
1341 |
1289 |
102.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5874.3 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 5648.7 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/cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.718 |
-0.059 |
| O2 |
0.000 |
-0.718 |
-0.059 |
| H3 |
0.787 |
0.897 |
0.469 |
| H4 |
-0.787 |
-0.897 |
0.469 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4370 | 0.9644 | 1.8730 |
O2 | 1.4370 | | 1.8730 | 0.9644 | H3 | 0.9644 | 1.8730 | | 2.3867 | H4 | 1.8730 | 0.9644 | 2.3867 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
100.671 |
|
O2 |
O1 |
H3 |
100.671 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.230 |
|
|
|
| 2 |
O |
-0.230 |
|
|
|
| 3 |
H |
0.230 |
|
|
|
| 4 |
H |
0.230 |
|
|
|
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 |
1.809 |
1.809 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.547 |
2.863 |
0.000 |
| y |
2.863 |
-11.182 |
0.000 |
| z |
0.000 |
0.000 |
-11.520 |
|
| Traceless |
| | x | y | z |
| x |
1.804 |
2.863 |
0.000 |
| y |
2.863 |
-0.649 |
0.000 |
| z |
0.000 |
0.000 |
-1.155 |
|
| Polar |
| 3z2-r2 | -2.310 |
| x2-y2 | 1.635 |
| xy | 2.863 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.607 |
0.277 |
0.000 |
| y |
0.277 |
2.320 |
0.000 |
| z |
0.000 |
0.000 |
1.319 |
<r2> (average value of r
2) Å
2
| <r2> |
18.318 |
| (<r2>)1/2 |
4.280 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVTZ
| | hartrees |
| Energy at 0K | -151.550186 |
| Energy at 298.15K | |
| HF Energy | -151.550186 |
| Nuclear repulsion energy | 36.936206 |
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/cc-pVTZ
| 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 |
3832 |
3685 |
0.00 |
|
|
|
| 2 |
Ag |
1545 |
1486 |
0.00 |
|
|
|
| 3 |
Ag |
986 |
948 |
0.00 |
|
|
|
| 4 |
Au |
304i |
292i |
268.08 |
|
|
|
| 5 |
Bu |
3839 |
3692 |
98.41 |
|
|
|
| 6 |
Bu |
1252 |
1204 |
133.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5574.8 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 5360.8 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/cc-pVTZ
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 |
0.874 |
0.000 |
| H4 |
-0.951 |
-0.874 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4483 | 0.9628 | 1.8597 |
O2 | 1.4483 | | 1.8597 | 0.9628 | H3 | 0.9628 | 1.8597 | | 2.5833 | H4 | 1.8597 | 0.9628 | 2.5833 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
98.952 |
|
O2 |
O1 |
H3 |
98.952 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.225 |
|
|
|
| 2 |
O |
-0.225 |
|
|
|
| 3 |
H |
0.225 |
|
|
|
| 4 |
H |
0.225 |
|
|
|
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 |
-8.059 |
3.406 |
0.000 |
| y |
3.406 |
-11.313 |
0.000 |
| z |
0.000 |
0.000 |
-12.708 |
|
| Traceless |
| | x | y | z |
| x |
3.952 |
3.406 |
0.000 |
| y |
3.406 |
-0.930 |
0.000 |
| z |
0.000 |
0.000 |
-3.022 |
|
| Polar |
| 3z2-r2 | -6.045 |
| x2-y2 | 3.255 |
| xy | 3.406 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.818 |
0.291 |
0.000 |
| y |
0.291 |
2.308 |
0.000 |
| z |
0.000 |
0.000 |
1.085 |
<r2> (average value of r
2) Å
2
| <r2> |
18.406 |
| (<r2>)1/2 |
4.290 |