Jump to
S1C2
Energy calculated at HF/3-21G*
| hartrees |
Energy at 0K | -149.945820 |
Energy at 298.15K | -149.947746 |
HF Energy | -149.945820 |
Nuclear repulsion energy | 36.393365 |
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/3-21G*
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 |
3827 |
3454 |
0.00 |
158.36 |
0.35 |
0.52 |
2 |
A |
1644 |
1484 |
0.00 |
9.56 |
0.75 |
0.86 |
3 |
A |
1168 |
1054 |
0.00 |
28.91 |
0.28 |
0.44 |
4 |
A |
89 |
80 |
444.42 |
0.00 |
0.75 |
0.86 |
5 |
B |
3844 |
3470 |
86.30 |
0.00 |
0.75 |
0.86 |
6 |
B |
1278 |
1153 |
150.80 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5924.9 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 5347.8 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/3-21G*
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.737 |
-0.000 |
O2 |
0.000 |
-0.737 |
-0.000 |
H3 |
0.957 |
0.896 |
0.000 |
H4 |
-0.957 |
-0.896 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4730 | 0.9703 | 1.8925 |
O2 | 1.4730 | | 1.8925 | 0.9703 | H3 | 0.9703 | 1.8925 | | 2.6223 | H4 | 1.8925 | 0.9703 | 2.6223 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
99.469 |
|
O2 |
O1 |
H3 |
99.469 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.418 |
|
|
|
2 |
O |
-0.418 |
|
|
|
3 |
H |
0.418 |
|
|
|
4 |
H |
0.418 |
|
|
|
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 |
0.000 |
0.000 |
0.002 |
0.002 |
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-7.567 |
3.994 |
0.000 |
y |
3.994 |
-11.020 |
0.000 |
z |
0.000 |
0.000 |
-12.116 |
|
Traceless |
| x | y | z |
x |
4.001 |
3.994 |
0.000 |
y |
3.994 |
-1.179 |
0.000 |
z |
0.000 |
0.000 |
-2.822 |
|
Polar |
3z2-r2 | -5.645 |
x2-y2 | 3.453 |
xy | 3.994 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.361 |
0.513 |
0.000 |
y |
0.513 |
2.092 |
0.000 |
z |
0.000 |
0.000 |
0.190 |
<r2> (average value of r
2) Å
2
<r2> |
18.509 |
(<r2>)1/2 |
4.302 |
Jump to
S1C1
Energy calculated at HF/3-21G*
| hartrees |
Energy at 0K | -149.945820 |
Energy at 298.15K | -149.947739 |
HF Energy | -149.945820 |
Nuclear repulsion energy | 36.386788 |
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/3-21G*
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 |
3828 |
3455 |
0.00 |
|
|
|
2 |
Ag |
1644 |
1484 |
0.00 |
|
|
|
3 |
Ag |
1167 |
1053 |
0.00 |
|
|
|
4 |
Au |
85 |
77 |
444.38 |
|
|
|
5 |
Bu |
3845 |
3470 |
86.29 |
|
|
|
6 |
Bu |
1277 |
1153 |
150.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5922.6 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 5345.7 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 HF/3-21G*
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.737 |
0.000 |
O2 |
0.000 |
-0.737 |
0.000 |
H3 |
0.957 |
0.896 |
0.000 |
H4 |
-0.957 |
-0.896 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4734 | 0.9703 | 1.8926 |
O2 | 1.4734 | | 1.8926 | 0.9703 | H3 | 0.9703 | 1.8926 | | 2.6222 | H4 | 1.8926 | 0.9703 | 2.6222 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
99.451 |
|
O2 |
O1 |
H3 |
99.451 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.418 |
|
|
|
2 |
O |
-0.418 |
|
|
|
3 |
H |
0.418 |
|
|
|
4 |
H |
0.418 |
|
|
|
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 |
-7.567 |
3.994 |
0.000 |
y |
3.994 |
-11.020 |
0.000 |
z |
0.000 |
0.000 |
-12.116 |
|
Traceless |
| x | y | z |
x |
4.001 |
3.994 |
0.000 |
y |
3.994 |
-1.179 |
0.000 |
z |
0.000 |
0.000 |
-2.822 |
|
Polar |
3z2-r2 | -5.645 |
x2-y2 | 3.453 |
xy | 3.994 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.361 |
0.513 |
0.000 |
y |
0.513 |
2.094 |
0.000 |
z |
0.000 |
0.000 |
0.190 |
<r2> (average value of r
2) Å
2
<r2> |
18.514 |
(<r2>)1/2 |
4.303 |