Jump to
S1C2
Energy calculated at LSDA/3-21G
| hartrees |
Energy at 0K | -149.971230 |
Energy at 298.15K | -149.973006 |
HF Energy | -149.971230 |
Nuclear repulsion energy | 35.365979 |
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 LSDA/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 |
3351 |
3296 |
0.00 |
|
|
|
2 |
A |
1458 |
1434 |
0.00 |
|
|
|
3 |
A |
1007 |
991 |
0.00 |
|
|
|
4 |
A |
30 |
30 |
351.09 |
|
|
|
5 |
B |
3380 |
3325 |
15.03 |
|
|
|
6 |
B |
1132 |
1113 |
159.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5178.9 cm
-1
Scaled (by 0.9836) Zero Point Vibrational Energy (zpe) 5094.0 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 LSDA/3-21G
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.758 |
-0.002 |
O2 |
0.000 |
-0.758 |
-0.002 |
H3 |
1.004 |
0.864 |
0.015 |
H4 |
-1.004 |
-0.864 |
0.015 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.5159 | 1.0096 | 1.9075 |
O2 | 1.5159 | | 1.9075 | 1.0096 | H3 | 1.0096 | 1.9075 | | 2.6489 | H4 | 1.9075 | 1.0096 | 2.6489 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
96.027 |
|
O2 |
O1 |
H3 |
96.027 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.374 |
|
|
|
2 |
O |
-0.374 |
|
|
|
3 |
H |
0.374 |
|
|
|
4 |
H |
0.374 |
|
|
|
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 |
0.066 |
0.066 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-7.541 |
3.582 |
0.000 |
y |
3.582 |
-11.105 |
0.000 |
z |
0.000 |
0.000 |
-12.180 |
|
Traceless |
| x | y | z |
x |
4.102 |
3.582 |
0.000 |
y |
3.582 |
-1.244 |
0.000 |
z |
0.000 |
0.000 |
-2.857 |
|
Polar |
3z2-r2 | -5.715 |
x2-y2 | 3.564 |
xy | 3.582 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.618 |
0.431 |
0.000 |
y |
0.431 |
1.795 |
0.000 |
z |
0.000 |
0.000 |
0.190 |
<r2> (average value of r
2) Å
2
<r2> |
19.118 |
(<r2>)1/2 |
4.372 |
Jump to
S1C1
Energy calculated at LSDA/3-21G
| hartrees |
Energy at 0K | -149.971230 |
Energy at 298.15K | |
HF Energy | -149.971230 |
Nuclear repulsion energy | 35.365326 |
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 LSDA/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 |
3351 |
3296 |
0.00 |
|
|
|
2 |
Ag |
1458 |
1434 |
0.00 |
|
|
|
3 |
Ag |
1007 |
990 |
0.00 |
|
|
|
4 |
Au |
23i |
22i |
351.25 |
|
|
|
5 |
Bu |
3381 |
3326 |
15.05 |
|
|
|
6 |
Bu |
1132 |
1113 |
159.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5152.9 cm
-1
Scaled (by 0.9836) Zero Point Vibrational Energy (zpe) 5068.4 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 LSDA/3-21G
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.758 |
0.000 |
O2 |
0.000 |
-0.758 |
0.000 |
H3 |
1.004 |
0.864 |
0.000 |
H4 |
-1.004 |
-0.864 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.5160 | 1.0095 | 1.9074 |
O2 | 1.5160 | | 1.9074 | 1.0095 | H3 | 1.0095 | 1.9074 | | 2.6489 | H4 | 1.9074 | 1.0095 | 2.6489 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
96.015 |
|
O2 |
O1 |
H3 |
96.015 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.374 |
|
|
|
2 |
O |
-0.374 |
|
|
|
3 |
H |
0.374 |
|
|
|
4 |
H |
0.374 |
|
|
|
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 |
-7.539 |
3.582 |
0.000 |
y |
3.582 |
-11.105 |
0.000 |
z |
0.000 |
0.000 |
-12.181 |
|
Traceless |
| x | y | z |
x |
4.104 |
3.582 |
0.000 |
y |
3.582 |
-1.245 |
0.000 |
z |
0.000 |
0.000 |
-2.858 |
|
Polar |
3z2-r2 | -5.717 |
x2-y2 | 3.566 |
xy | 3.582 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.618 |
0.431 |
0.000 |
y |
0.431 |
1.795 |
0.000 |
z |
0.000 |
0.000 |
0.189 |
<r2> (average value of r
2) Å
2
<r2> |
19.119 |
(<r2>)1/2 |
4.373 |