Jump to
S1C2
Energy calculated at HF/cc-pVQZ
| | hartrees |
| Energy at 0K | -150.852251 |
| Energy at 298.15K | -150.854630 |
| HF Energy | -150.852251 |
| Nuclear repulsion energy | 38.273870 |
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 HF/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 |
4137 |
3758 |
28.58 |
78.17 |
0.13 |
0.23 |
| 2 |
A |
1610 |
1462 |
0.53 |
2.90 |
0.53 |
0.70 |
| 3 |
A |
1163 |
1056 |
0.88 |
26.24 |
0.26 |
0.41 |
| 4 |
A |
416 |
378 |
192.44 |
3.11 |
0.75 |
0.86 |
| 5 |
B |
4136 |
3757 |
94.43 |
26.26 |
0.75 |
0.86 |
| 6 |
B |
1493 |
1356 |
105.86 |
0.96 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 6477.9 cm
-1
Scaled (by 0.9084) Zero Point Vibrational Energy (zpe) 5884.5 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 HF/cc-pVQZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.692 |
-0.058 |
| O2 |
0.000 |
-0.692 |
-0.058 |
| H3 |
0.757 |
0.905 |
0.460 |
| H4 |
-0.757 |
-0.905 |
0.460 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.3848 | 0.9412 | 1.8420 |
O2 | 1.3848 | | 1.8420 | 0.9412 | H3 | 0.9412 | 1.8420 | | 2.3598 | H4 | 1.8420 | 0.9412 | 2.3598 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
103.077 |
|
O2 |
O1 |
H3 |
103.077 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.268 |
|
|
|
| 2 |
O |
-0.268 |
|
|
|
| 3 |
H |
0.268 |
|
|
|
| 4 |
H |
0.268 |
|
|
|
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 |
1.889 |
1.889 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.552 |
3.011 |
0.000 |
| y |
3.011 |
-11.186 |
0.000 |
| z |
0.000 |
0.000 |
-11.427 |
|
| Traceless |
| | x | y | z |
| x |
1.754 |
3.011 |
0.000 |
| y |
3.011 |
-0.697 |
0.000 |
| z |
0.000 |
0.000 |
-1.057 |
|
| Polar |
| 3z2-r2 | -2.115 |
| x2-y2 | 1.634 |
| xy | 3.011 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.563 |
0.252 |
0.000 |
| y |
0.252 |
2.391 |
0.000 |
| z |
0.000 |
0.000 |
1.366 |
<r2> (average value of r
2) Å
2
| <r2> |
17.628 |
| (<r2>)1/2 |
4.199 |
Jump to
S1C1
Energy calculated at HF/cc-pVQZ
| | hartrees |
| Energy at 0K | -150.850316 |
| Energy at 298.15K | |
| HF Energy | -150.850316 |
| Nuclear repulsion energy | 38.139657 |
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 HF/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 |
4159 |
3778 |
0.00 |
|
|
|
| 2 |
Ag |
1705 |
1549 |
0.00 |
|
|
|
| 3 |
Ag |
1159 |
1053 |
0.00 |
|
|
|
| 4 |
Au |
325i |
295i |
302.12 |
|
|
|
| 5 |
Bu |
4168 |
3786 |
169.76 |
|
|
|
| 6 |
Bu |
1380 |
1254 |
135.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6123.1 cm
-1
Scaled (by 0.9084) Zero Point Vibrational Energy (zpe) 5562.2 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 HF/cc-pVQZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.697 |
0.000 |
| O2 |
0.000 |
-0.697 |
0.000 |
| H3 |
0.921 |
0.884 |
0.000 |
| H4 |
-0.921 |
-0.884 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.3937 | 0.9403 | 1.8297 |
O2 | 1.3937 | | 1.8297 | 0.9403 | H3 | 0.9403 | 1.8297 | | 2.5537 | H4 | 1.8297 | 0.9403 | 2.5537 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
101.470 |
|
O2 |
O1 |
H3 |
101.470 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/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 |
-8.042 |
3.608 |
0.000 |
| y |
3.608 |
-11.328 |
0.000 |
| z |
0.000 |
0.000 |
-12.627 |
|
| Traceless |
| | x | y | z |
| x |
3.936 |
3.608 |
0.000 |
| y |
3.608 |
-0.994 |
0.000 |
| z |
0.000 |
0.000 |
-2.942 |
|
| Polar |
| 3z2-r2 | -5.883 |
| x2-y2 | 3.286 |
| xy | 3.608 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.726 |
0.276 |
0.000 |
| y |
0.276 |
2.391 |
0.000 |
| z |
0.000 |
0.000 |
1.201 |
<r2> (average value of r
2) Å
2
| <r2> |
17.692 |
| (<r2>)1/2 |
4.206 |