Jump to
S1C2
Energy calculated at HSEh1PBE/Def2TZVPP
| hartrees |
Energy at 0K | -151.471550 |
Energy at 298.15K | -151.473865 |
HF Energy | -151.471550 |
Nuclear repulsion energy | 37.274801 |
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/Def2TZVPP
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 |
3825 |
3825 |
14.07 |
86.79 |
0.13 |
0.24 |
2 |
A |
1465 |
1465 |
0.33 |
6.39 |
0.51 |
0.68 |
3 |
A |
999 |
999 |
0.93 |
14.08 |
0.24 |
0.39 |
4 |
A |
386 |
386 |
175.94 |
3.74 |
0.75 |
0.86 |
5 |
B |
3825 |
3825 |
53.75 |
31.07 |
0.75 |
0.86 |
6 |
B |
1353 |
1353 |
100.39 |
1.89 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5925.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5925.9 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/Def2TZVPP
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.714 |
-0.058 |
O2 |
0.000 |
-0.714 |
-0.058 |
H3 |
0.786 |
0.899 |
0.465 |
H4 |
-0.786 |
-0.899 |
0.465 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4274 | 0.9625 | 1.8691 |
O2 | 1.4274 | | 1.8691 | 0.9625 | H3 | 0.9625 | 1.8691 | | 2.3891 | H4 | 1.8691 | 0.9625 | 2.3891 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
101.112 |
|
O2 |
O1 |
H3 |
101.112 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.225 |
|
|
|
2 |
O |
-0.225 |
|
|
|
3 |
H |
0.225 |
|
|
|
4 |
H |
0.225 |
|
|
|
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 |
1.818 |
1.818 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-9.659 |
2.932 |
0.000 |
y |
2.932 |
-11.334 |
0.000 |
z |
0.000 |
0.000 |
-11.687 |
|
Traceless |
| x | y | z |
x |
1.852 |
2.932 |
0.000 |
y |
2.932 |
-0.661 |
0.000 |
z |
0.000 |
0.000 |
-1.190 |
|
Polar |
3z2-r2 | -2.380 |
x2-y2 | 1.675 |
xy | 2.932 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.669 |
0.260 |
0.000 |
y |
0.260 |
2.370 |
0.000 |
z |
0.000 |
0.000 |
1.420 |
<r2> (average value of r
2) Å
2
<r2> |
18.294 |
(<r2>)1/2 |
4.277 |
Jump to
S1C1
Energy calculated at HSEh1PBE/Def2TZVPP
| hartrees |
Energy at 0K | -151.469813 |
Energy at 298.15K | |
HF Energy | -151.469813 |
Nuclear repulsion energy | 37.119880 |
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/Def2TZVPP
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 |
3859 |
3859 |
0.00 |
|
|
|
2 |
Ag |
1558 |
1558 |
0.00 |
|
|
|
3 |
Ag |
1000 |
1000 |
0.00 |
|
|
|
4 |
Au |
306i |
306i |
273.82 |
|
|
|
5 |
Bu |
3867 |
3867 |
107.53 |
|
|
|
6 |
Bu |
1264 |
1264 |
132.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5620.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5620.7 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/Def2TZVPP
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.719 |
0.000 |
O2 |
0.000 |
-0.719 |
0.000 |
H3 |
0.948 |
0.876 |
0.000 |
H4 |
-0.948 |
-0.876 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4386 | 0.9610 | 1.8556 |
O2 | 1.4386 | | 1.8556 | 0.9610 | H3 | 0.9610 | 1.8556 | | 2.5814 | H4 | 1.8556 | 0.9610 | 2.5814 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
99.364 |
|
O2 |
O1 |
H3 |
99.364 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.226 |
|
|
|
2 |
O |
-0.226 |
|
|
|
3 |
H |
0.226 |
|
|
|
4 |
H |
0.226 |
|
|
|
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 |
-8.172 |
3.479 |
0.000 |
y |
3.479 |
-11.470 |
0.000 |
z |
0.000 |
0.000 |
-12.877 |
|
Traceless |
| x | y | z |
x |
4.001 |
3.479 |
0.000 |
y |
3.479 |
-0.945 |
0.000 |
z |
0.000 |
0.000 |
-3.056 |
|
Polar |
3z2-r2 | -6.112 |
x2-y2 | 3.298 |
xy | 3.479 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.843 |
0.273 |
0.000 |
y |
0.273 |
2.353 |
0.000 |
z |
0.000 |
0.000 |
1.233 |
<r2> (average value of r
2) Å
2
<r2> |
18.381 |
(<r2>)1/2 |
4.287 |