Jump to
S1C2
Energy calculated at LSDA/STO-3G
| hartrees |
Energy at 0K | -148.695008 |
Energy at 298.15K | -148.697061 |
HF Energy | -148.695008 |
Nuclear repulsion energy | 36.006582 |
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/STO-3G
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 |
3512 |
3145 |
30.64 |
|
|
|
2 |
A |
1475 |
1321 |
0.09 |
|
|
|
3 |
A |
1200 |
1074 |
0.10 |
|
|
|
4 |
A |
199 |
178 |
91.10 |
|
|
|
5 |
B |
3522 |
3154 |
65.89 |
|
|
|
6 |
B |
1359 |
1217 |
30.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5633.3 cm
-1
Scaled (by 0.8955) Zero Point Vibrational Energy (zpe) 5044.6 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/STO-3G
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.728 |
-0.060 |
O2 |
0.000 |
-0.728 |
-0.060 |
H3 |
0.882 |
0.885 |
0.479 |
H4 |
-0.882 |
-0.885 |
0.479 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4551 | 1.0453 | 1.9155 |
O2 | 1.4551 | | 1.9155 | 1.0453 | H3 | 1.0453 | 1.9155 | | 2.4988 | H4 | 1.9155 | 1.0453 | 2.4988 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
98.678 |
|
O2 |
O1 |
H3 |
98.678 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.177 |
|
|
|
2 |
O |
-0.177 |
|
|
|
3 |
H |
0.177 |
|
|
|
4 |
H |
0.177 |
|
|
|
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 |
1.374 |
1.374 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-8.490 |
1.980 |
0.000 |
y |
1.980 |
-10.215 |
0.000 |
z |
0.000 |
0.000 |
-10.091 |
|
Traceless |
| x | y | z |
x |
1.663 |
1.980 |
0.000 |
y |
1.980 |
-0.924 |
0.000 |
z |
0.000 |
0.000 |
-0.739 |
|
Polar |
3z2-r2 | -1.478 |
x2-y2 | 1.724 |
xy | 1.980 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.973 |
0.460 |
0.000 |
y |
0.460 |
1.184 |
0.000 |
z |
0.000 |
0.000 |
0.340 |
<r2> (average value of r
2) Å
2
<r2> |
18.103 |
(<r2>)1/2 |
4.255 |
Jump to
S1C1
Energy calculated at LSDA/STO-3G
| hartrees |
Energy at 0K | -148.694922 |
Energy at 298.15K | -148.696835 |
HF Energy | -148.694922 |
Nuclear repulsion energy | 35.907848 |
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/STO-3G
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 |
3590 |
3215 |
0.00 |
|
|
|
2 |
Ag |
1644 |
1472 |
0.00 |
|
|
|
3 |
Ag |
1232 |
1103 |
0.00 |
|
|
|
4 |
Au |
104 |
93 |
152.27 |
|
|
|
5 |
Bu |
3618 |
3240 |
46.96 |
|
|
|
6 |
Bu |
1273 |
1140 |
55.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5729.8 cm
-1
Scaled (by 0.8955) Zero Point Vibrational Energy (zpe) 5131.0 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/STO-3G
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.733 |
0.000 |
O2 |
0.000 |
-0.733 |
0.000 |
H3 |
1.034 |
0.849 |
0.000 |
H4 |
-1.034 |
-0.849 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4666 | 1.0404 | 1.8900 |
O2 | 1.4666 | | 1.8900 | 1.0404 | H3 | 1.0404 | 1.8900 | | 2.6755 | H4 | 1.8900 | 1.0404 | 2.6755 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
96.371 |
|
O2 |
O1 |
H3 |
96.371 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.184 |
|
|
|
2 |
O |
-0.184 |
|
|
|
3 |
H |
0.184 |
|
|
|
4 |
H |
0.184 |
|
|
|
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 |
-7.540 |
2.307 |
0.000 |
y |
2.307 |
-10.311 |
0.000 |
z |
0.000 |
0.000 |
-10.784 |
|
Traceless |
| x | y | z |
x |
3.007 |
2.307 |
0.000 |
y |
2.307 |
-1.149 |
0.000 |
z |
0.000 |
0.000 |
-1.858 |
|
Polar |
3z2-r2 | -3.717 |
x2-y2 | 2.771 |
xy | 2.307 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.256 |
0.457 |
0.000 |
y |
0.457 |
1.145 |
0.000 |
z |
0.000 |
0.000 |
0.032 |
<r2> (average value of r
2) Å
2
<r2> |
18.144 |
(<r2>)1/2 |
4.260 |