Jump to
S1C2
Energy calculated at B97D3/6-31G*
| | hartrees |
| Energy at 0K | -151.454270 |
| Energy at 298.15K | -151.456507 |
| HF Energy | -151.454270 |
| Nuclear repulsion energy | 36.362244 |
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 B97D3/6-31G*
| 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 |
3612 |
3541 |
3.02 |
93.48 |
0.19 |
0.32 |
| 2 |
A |
1433 |
1405 |
0.55 |
11.15 |
0.61 |
0.76 |
| 3 |
A |
893 |
876 |
1.76 |
9.92 |
0.27 |
0.42 |
| 4 |
A |
344 |
338 |
191.02 |
7.78 |
0.75 |
0.86 |
| 5 |
B |
3614 |
3544 |
20.07 |
39.12 |
0.75 |
0.86 |
| 6 |
B |
1299 |
1274 |
101.47 |
2.94 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5598.2 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 5488.5 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 B97D3/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.736 |
-0.055 |
| O2 |
0.000 |
-0.736 |
-0.055 |
| H3 |
0.829 |
0.888 |
0.441 |
| H4 |
-0.829 |
-0.888 |
0.441 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4718 | 0.9784 | 1.8901 |
O2 | 1.4718 | | 1.8901 | 0.9784 | H3 | 0.9784 | 1.8901 | | 2.4306 | H4 | 1.8901 | 0.9784 | 2.4306 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
98.974 |
|
O2 |
O1 |
H3 |
98.974 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.410 |
|
|
|
| 2 |
O |
-0.410 |
|
|
|
| 3 |
H |
0.410 |
|
|
|
| 4 |
H |
0.410 |
|
|
|
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 |
1.760 |
1.760 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.158 |
2.935 |
0.000 |
| y |
2.935 |
-11.031 |
0.000 |
| z |
0.000 |
0.000 |
-11.519 |
|
| Traceless |
| | x | y | z |
| x |
2.117 |
2.935 |
0.000 |
| y |
2.935 |
-0.692 |
0.000 |
| z |
0.000 |
0.000 |
-1.425 |
|
| Polar |
| 3z2-r2 | -2.850 |
| x2-y2 | 1.873 |
| xy | 2.935 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.433 |
0.328 |
0.000 |
| y |
0.328 |
2.062 |
0.000 |
| z |
0.000 |
0.000 |
0.946 |
<r2> (average value of r
2) Å
2
| <r2> |
18.658 |
| (<r2>)1/2 |
4.319 |
Jump to
S1C1
Energy calculated at B97D3/6-31G*
| | hartrees |
| Energy at 0K | -151.453138 |
| Energy at 298.15K | |
| HF Energy | -151.453138 |
| Nuclear repulsion energy | 36.194381 |
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 B97D3/6-31G*
| 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 |
3651 |
3579 |
0.00 |
|
|
|
| 2 |
Ag |
1530 |
1500 |
0.00 |
|
|
|
| 3 |
Ag |
899 |
881 |
0.00 |
|
|
|
| 4 |
Au |
252i |
247i |
287.61 |
|
|
|
| 5 |
Bu |
3664 |
3592 |
47.53 |
|
|
|
| 6 |
Bu |
1237 |
1213 |
134.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5364.5 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 5259.4 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 B97D3/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.742 |
0.000 |
| O2 |
0.000 |
-0.742 |
0.000 |
| H3 |
0.969 |
0.866 |
0.000 |
| H4 |
-0.969 |
-0.866 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4841 | 0.9770 | 1.8777 |
O2 | 1.4841 | | 1.8777 | 0.9770 | H3 | 0.9770 | 1.8777 | | 2.5996 | H4 | 1.8777 | 0.9770 | 2.5996 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
97.298 |
|
O2 |
O1 |
H3 |
97.298 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.415 |
|
|
|
| 2 |
O |
-0.415 |
|
|
|
| 3 |
H |
0.415 |
|
|
|
| 4 |
H |
0.415 |
|
|
|
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 |
-7.865 |
3.394 |
0.000 |
| y |
3.394 |
-11.150 |
0.000 |
| z |
0.000 |
0.000 |
-12.542 |
|
| Traceless |
| | x | y | z |
| x |
3.981 |
3.394 |
0.000 |
| y |
3.394 |
-0.946 |
0.000 |
| z |
0.000 |
0.000 |
-3.034 |
|
| Polar |
| 3z2-r2 | -6.069 |
| x2-y2 | 3.285 |
| xy | 3.394 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.667 |
0.340 |
0.000 |
| y |
0.340 |
2.065 |
0.000 |
| z |
0.000 |
0.000 |
0.693 |
<r2> (average value of r
2) Å
2
| <r2> |
18.760 |
| (<r2>)1/2 |
4.331 |