Jump to
S1C2
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -151.461407 |
Energy at 298.15K | -151.463757 |
HF Energy | -151.461407 |
Nuclear repulsion energy | 37.329100 |
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 HSEh1PBE/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 |
3831 |
3831 |
16.43 |
89.85 |
0.12 |
0.21 |
2 |
A |
1468 |
1468 |
0.35 |
6.46 |
0.36 |
0.52 |
3 |
A |
1001 |
1001 |
0.68 |
14.03 |
0.23 |
0.37 |
4 |
A |
420 |
420 |
165.31 |
0.84 |
0.73 |
0.85 |
5 |
B |
3831 |
3831 |
55.96 |
29.36 |
0.75 |
0.86 |
6 |
B |
1368 |
1368 |
97.83 |
1.35 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5959.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5959.9 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.712 |
-0.060 |
O2 |
0.000 |
-0.712 |
-0.060 |
H3 |
0.773 |
0.902 |
0.481 |
H4 |
-0.773 |
-0.902 |
0.481 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4240 | 0.9627 | 1.8696 |
O2 | 1.4240 | | 1.8696 | 0.9627 | H3 | 0.9627 | 1.8696 | | 2.3756 | H4 | 1.8696 | 0.9627 | 2.3756 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
101.379 |
|
O2 |
O1 |
H3 |
101.379 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.242 |
|
|
|
2 |
O |
-0.242 |
|
|
|
3 |
H |
0.242 |
|
|
|
4 |
H |
0.242 |
|
|
|
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 |
1.830 |
1.830 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-9.920 |
2.898 |
0.000 |
y |
2.898 |
-11.403 |
0.000 |
z |
0.000 |
0.000 |
-11.803 |
|
Traceless |
| x | y | z |
x |
1.683 |
2.898 |
0.000 |
y |
2.898 |
-0.541 |
0.000 |
z |
0.000 |
0.000 |
-1.142 |
|
Polar |
3z2-r2 | -2.283 |
x2-y2 | 1.483 |
xy | 2.898 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.866 |
0.226 |
0.000 |
y |
0.226 |
2.558 |
0.000 |
z |
0.000 |
0.000 |
1.745 |
<r2> (average value of r
2) Å
2
<r2> |
18.351 |
(<r2>)1/2 |
4.284 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -151.459264 |
Energy at 298.15K | |
HF Energy | -151.459264 |
Nuclear repulsion energy | 37.176115 |
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 HSEh1PBE/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 |
3870 |
3870 |
0.00 |
|
|
|
2 |
Ag |
1571 |
1571 |
0.00 |
|
|
|
3 |
Ag |
1002 |
1002 |
0.00 |
|
|
|
4 |
Au |
322i |
322i |
261.85 |
|
|
|
5 |
Bu |
3879 |
3879 |
114.66 |
|
|
|
6 |
Bu |
1273 |
1273 |
132.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5636.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5636.3 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.718 |
0.000 |
O2 |
0.000 |
-0.718 |
0.000 |
H3 |
0.948 |
0.878 |
0.000 |
H4 |
-0.948 |
-0.878 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4352 | 0.9610 | 1.8558 |
O2 | 1.4352 | | 1.8558 | 0.9610 | H3 | 0.9610 | 1.8558 | | 2.5836 | H4 | 1.8558 | 0.9610 | 2.5836 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
99.613 |
|
O2 |
O1 |
H3 |
99.613 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.249 |
|
|
|
2 |
O |
-0.249 |
|
|
|
3 |
H |
0.249 |
|
|
|
4 |
H |
0.249 |
|
|
|
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 |
3.493 |
0.000 |
y |
3.493 |
-11.551 |
0.000 |
z |
0.000 |
0.000 |
-13.153 |
|
Traceless |
| x | y | z |
x |
4.093 |
3.493 |
0.000 |
y |
3.493 |
-0.845 |
0.000 |
z |
0.000 |
0.000 |
-3.248 |
|
Polar |
3z2-r2 | -6.496 |
x2-y2 | 3.292 |
xy | 3.493 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.958 |
0.247 |
0.000 |
y |
0.247 |
2.562 |
0.000 |
z |
0.000 |
0.000 |
1.649 |
<r2> (average value of r
2) Å
2
<r2> |
18.439 |
(<r2>)1/2 |
4.294 |