Jump to
S1C2
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -151.475917 |
| Energy at 298.15K | -151.478205 |
| HF Energy | -151.475917 |
| Nuclear repulsion energy | 36.950625 |
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 B3PW91/6-31G*
| 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 |
3745 |
3583 |
7.21 |
|
|
|
| 2 |
A |
1484 |
1420 |
0.46 |
|
|
|
| 3 |
A |
985 |
943 |
1.79 |
|
|
|
| 4 |
A |
368 |
352 |
205.32 |
|
|
|
| 5 |
B |
3747 |
3585 |
35.19 |
|
|
|
| 6 |
B |
1350 |
1292 |
109.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5839.9 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 5587.1 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 B3PW91/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.721 |
-0.055 |
| O2 |
0.000 |
-0.721 |
-0.055 |
| H3 |
0.817 |
0.889 |
0.442 |
| H4 |
-0.817 |
-0.889 |
0.442 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4415 | 0.9714 | 1.8728 |
O2 | 1.4415 | | 1.8728 | 0.9714 | H3 | 0.9714 | 1.8728 | | 2.4155 | H4 | 1.8728 | 0.9714 | 2.4155 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
99.989 |
|
O2 |
O1 |
H3 |
99.989 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.428 |
|
|
|
| 2 |
O |
-0.428 |
|
|
|
| 3 |
H |
0.428 |
|
|
|
| 4 |
H |
0.428 |
|
|
|
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 |
1.835 |
1.835 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.004 |
-0.000 |
1.919 |
1.919 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.162 |
3.023 |
0.000 |
| y |
3.023 |
-11.062 |
0.000 |
| z |
0.000 |
0.000 |
-11.495 |
|
| Traceless |
| | x | y | z |
| x |
2.116 |
3.023 |
0.000 |
| y |
3.023 |
-0.733 |
0.000 |
| z |
0.000 |
0.000 |
-1.383 |
|
| Polar |
| 3z2-r2 | -2.765 |
| x2-y2 | 1.899 |
| xy | 3.023 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.366 |
0.325 |
0.000 |
| y |
0.325 |
2.000 |
0.000 |
| z |
0.000 |
0.000 |
0.925 |
<r2> (average value of r
2) Å
2
| <r2> |
18.272 |
| (<r2>)1/2 |
4.275 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -151.474619 |
| Energy at 298.15K | |
| HF Energy | -151.474619 |
| Nuclear repulsion energy | 36.786607 |
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 B3PW91/6-31G*
| 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 |
3779 |
3615 |
0.00 |
|
|
|
| 2 |
Ag |
1577 |
1509 |
0.00 |
|
|
|
| 3 |
Ag |
988 |
945 |
0.00 |
|
|
|
| 4 |
Au |
274i |
262i |
311.62 |
|
|
|
| 5 |
Bu |
3792 |
3628 |
75.33 |
|
|
|
| 6 |
Bu |
1275 |
1220 |
143.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5568.1 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 5327.0 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 B3PW91/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.727 |
0.000 |
| O2 |
0.000 |
-0.727 |
0.000 |
| H3 |
0.960 |
0.867 |
0.000 |
| H4 |
-0.960 |
-0.867 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4533 | 0.9702 | 1.8603 |
O2 | 1.4533 | | 1.8603 | 0.9702 | H3 | 0.9702 | 1.8603 | | 2.5868 | H4 | 1.8603 | 0.9702 | 2.5868 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
98.301 |
|
O2 |
O1 |
H3 |
98.301 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.433 |
|
|
|
| 2 |
O |
-0.433 |
|
|
|
| 3 |
H |
0.433 |
|
|
|
| 4 |
H |
0.433 |
|
|
|
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 |
-7.820 |
3.514 |
0.000 |
| y |
3.514 |
-11.189 |
0.000 |
| z |
0.000 |
0.000 |
-12.550 |
|
| Traceless |
| | x | y | z |
| x |
4.049 |
3.514 |
0.000 |
| y |
3.514 |
-1.004 |
0.000 |
| z |
0.000 |
0.000 |
-3.045 |
|
| Polar |
| 3z2-r2 | -6.090 |
| x2-y2 | 3.369 |
| xy | 3.514 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.588 |
0.339 |
0.000 |
| y |
0.339 |
2.008 |
0.000 |
| z |
0.000 |
0.000 |
0.686 |
<r2> (average value of r
2) Å
2
| <r2> |
18.365 |
| (<r2>)1/2 |
4.285 |