Jump to
S1C2
Energy calculated at B3LYP/cc-pVQZ
| | hartrees |
| Energy at 0K | -151.626743 |
| Energy at 298.15K | -151.629042 |
| HF Energy | -151.626743 |
| Nuclear repulsion energy | 36.860117 |
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 B3LYP/cc-pVQZ
| 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 |
3766 |
3649 |
12.80 |
88.71 |
0.13 |
0.23 |
| 2 |
A |
1439 |
1394 |
0.57 |
5.67 |
0.44 |
0.61 |
| 3 |
A |
950 |
920 |
0.83 |
14.62 |
0.23 |
0.37 |
| 4 |
A |
381 |
369 |
168.38 |
4.15 |
0.74 |
0.85 |
| 5 |
B |
3764 |
3647 |
53.08 |
30.26 |
0.75 |
0.86 |
| 6 |
B |
1327 |
1286 |
101.25 |
1.45 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5813.7 cm
-1
Scaled (by 0.9688) Zero Point Vibrational Energy (zpe) 5632.3 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 B3LYP/cc-pVQZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.725 |
-0.058 |
| O2 |
0.000 |
-0.725 |
-0.058 |
| H3 |
0.790 |
0.903 |
0.466 |
| H4 |
-0.790 |
-0.903 |
0.466 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4490 | 0.9650 | 1.8841 |
O2 | 1.4490 | | 1.8841 | 0.9650 | H3 | 0.9650 | 1.8841 | | 2.4008 | H4 | 1.8841 | 0.9650 | 2.4008 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
100.688 |
|
O2 |
O1 |
H3 |
100.688 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.267 |
|
|
|
| 2 |
O |
-0.267 |
|
|
|
| 3 |
H |
0.267 |
|
|
|
| 4 |
H |
0.267 |
|
|
|
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 |
1.777 |
1.777 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.734 |
2.906 |
0.000 |
| y |
2.906 |
-11.389 |
0.000 |
| z |
0.000 |
0.000 |
-11.757 |
|
| Traceless |
| | x | y | z |
| x |
1.839 |
2.906 |
0.000 |
| y |
2.906 |
-0.643 |
0.000 |
| z |
0.000 |
0.000 |
-1.196 |
|
| Polar |
| 3z2-r2 | -2.392 |
| x2-y2 | 1.654 |
| xy | 2.906 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.786 |
0.263 |
0.000 |
| y |
0.263 |
2.552 |
0.000 |
| z |
0.000 |
0.000 |
1.533 |
<r2> (average value of r
2) Å
2
| <r2> |
18.614 |
| (<r2>)1/2 |
4.314 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVQZ
| | hartrees |
| Energy at 0K | -151.625106 |
| Energy at 298.15K | |
| HF Energy | -151.625106 |
| Nuclear repulsion energy | 36.708487 |
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 B3LYP/cc-pVQZ
| 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 |
3798 |
3680 |
0.00 |
|
|
|
| 2 |
Ag |
1532 |
1485 |
0.00 |
|
|
|
| 3 |
Ag |
951 |
921 |
0.00 |
|
|
|
| 4 |
Au |
293i |
284i |
261.66 |
|
|
|
| 5 |
Bu |
3805 |
3686 |
101.98 |
|
|
|
| 6 |
Bu |
1242 |
1203 |
132.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5517.8 cm
-1
Scaled (by 0.9688) Zero Point Vibrational Energy (zpe) 5345.6 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 B3LYP/cc-pVQZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.730 |
0.000 |
| O2 |
0.000 |
-0.730 |
0.000 |
| H3 |
0.952 |
0.881 |
0.000 |
| H4 |
-0.952 |
-0.881 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4602 | 0.9637 | 1.8711 |
O2 | 1.4602 | | 1.8711 | 0.9637 | H3 | 0.9637 | 1.8711 | | 2.5938 | H4 | 1.8711 | 0.9637 | 2.5938 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
99.000 |
|
O2 |
O1 |
H3 |
99.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.269 |
|
|
|
| 2 |
O |
-0.269 |
|
|
|
| 3 |
H |
0.269 |
|
|
|
| 4 |
H |
0.269 |
|
|
|
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 |
-8.260 |
3.445 |
0.000 |
| y |
3.445 |
-11.520 |
0.000 |
| z |
0.000 |
0.000 |
-12.934 |
|
| Traceless |
| | x | y | z |
| x |
3.968 |
3.445 |
0.000 |
| y |
3.445 |
-0.923 |
0.000 |
| z |
0.000 |
0.000 |
-3.044 |
|
| Polar |
| 3z2-r2 | -6.088 |
| x2-y2 | 3.261 |
| xy | 3.445 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.969 |
0.277 |
0.000 |
| y |
0.277 |
2.535 |
0.000 |
| z |
0.000 |
0.000 |
1.340 |
<r2> (average value of r
2) Å
2
| <r2> |
18.703 |
| (<r2>)1/2 |
4.325 |