Jump to
S1C2
Energy calculated at HF/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -150.836745 |
Energy at 298.15K | -150.839143 |
HF Energy | -150.836745 |
Nuclear repulsion energy | 38.311253 |
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/6-311+G(3df,2p)
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 |
4154 |
3775 |
30.71 |
79.93 |
0.12 |
0.22 |
2 |
A |
1613 |
1466 |
0.31 |
3.33 |
0.45 |
0.62 |
3 |
A |
1167 |
1060 |
0.77 |
26.55 |
0.26 |
0.41 |
4 |
A |
435 |
395 |
190.51 |
1.06 |
0.73 |
0.85 |
5 |
B |
4154 |
3775 |
95.25 |
25.96 |
0.75 |
0.86 |
6 |
B |
1503 |
1365 |
103.90 |
0.87 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 6513.1 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 5917.8 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 HF/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.691 |
-0.059 |
O2 |
0.000 |
-0.691 |
-0.059 |
H3 |
0.750 |
0.906 |
0.469 |
H4 |
-0.750 |
-0.906 |
0.469 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.3825 | 0.9416 | 1.8418 |
O2 | 1.3825 | | 1.8418 | 0.9416 | H3 | 0.9416 | 1.8418 | | 2.3527 | H4 | 1.8418 | 0.9416 | 2.3527 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
103.196 |
|
O2 |
O1 |
H3 |
103.196 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.228 |
|
|
|
2 |
O |
-0.228 |
|
|
|
3 |
H |
0.228 |
|
|
|
4 |
H |
0.228 |
|
|
|
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 |
1.917 |
1.917 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-9.704 |
3.020 |
0.000 |
y |
3.020 |
-11.208 |
0.000 |
z |
0.000 |
0.000 |
-11.521 |
|
Traceless |
| x | y | z |
x |
1.660 |
3.020 |
0.000 |
y |
3.020 |
-0.595 |
0.000 |
z |
0.000 |
0.000 |
-1.065 |
|
Polar |
3z2-r2 | -2.130 |
x2-y2 | 1.504 |
xy | 3.020 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.638 |
0.233 |
0.000 |
y |
0.233 |
2.441 |
0.000 |
z |
0.000 |
0.000 |
1.513 |
<r2> (average value of r
2) Å
2
<r2> |
17.659 |
(<r2>)1/2 |
4.202 |
Jump to
S1C1
Energy calculated at HF/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -150.834614 |
Energy at 298.15K | |
HF Energy | -150.834614 |
Nuclear repulsion energy | 38.179345 |
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/6-311+G(3df,2p)
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 |
4180 |
3798 |
0.00 |
|
|
|
2 |
Ag |
1718 |
1561 |
0.00 |
|
|
|
3 |
Ag |
1164 |
1057 |
0.00 |
|
|
|
4 |
Au |
325i |
295i |
301.87 |
|
|
|
5 |
Bu |
4189 |
3807 |
174.24 |
|
|
|
6 |
Bu |
1386 |
1259 |
135.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6156.0 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 5593.3 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 HF/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.696 |
0.000 |
O2 |
0.000 |
-0.696 |
0.000 |
H3 |
0.921 |
0.885 |
0.000 |
H4 |
-0.921 |
-0.885 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.3913 | 0.9406 | 1.8295 |
O2 | 1.3913 | | 1.8295 | 0.9406 | H3 | 0.9406 | 1.8295 | | 2.5550 | H4 | 1.8295 | 0.9406 | 2.5550 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
101.610 |
|
O2 |
O1 |
H3 |
101.610 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.238 |
|
|
|
2 |
O |
-0.238 |
|
|
|
3 |
H |
0.238 |
|
|
|
4 |
H |
0.238 |
|
|
|
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 |
-8.087 |
3.649 |
0.000 |
y |
3.649 |
-11.358 |
0.000 |
z |
0.000 |
0.000 |
-12.825 |
|
Traceless |
| x | y | z |
x |
4.005 |
3.649 |
0.000 |
y |
3.649 |
-0.903 |
0.000 |
z |
0.000 |
0.000 |
-3.102 |
|
Polar |
3z2-r2 | -6.205 |
x2-y2 | 3.272 |
xy | 3.649 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.741 |
0.263 |
0.000 |
y |
0.263 |
2.463 |
0.000 |
z |
0.000 |
0.000 |
1.414 |
<r2> (average value of r
2) Å
2
<r2> |
17.725 |
(<r2>)1/2 |
4.210 |