Jump to
S1C2
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -150.829757 |
| Energy at 298.15K | -150.832067 |
| HF Energy | -150.829757 |
| Nuclear repulsion energy | 36.961377 |
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/6-31+G**
| 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 |
3672 |
3617 |
12.69 |
|
|
|
| 2 |
A |
1404 |
1383 |
0.10 |
|
|
|
| 3 |
A |
970 |
955 |
1.28 |
|
|
|
| 4 |
A |
397 |
391 |
225.02 |
|
|
|
| 5 |
B |
3671 |
3616 |
64.96 |
|
|
|
| 6 |
B |
1263 |
1244 |
101.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5688.2 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 5602.9 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 LSDA/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.717 |
-0.055 |
| O2 |
0.000 |
-0.717 |
-0.055 |
| H3 |
0.827 |
0.897 |
0.441 |
| H4 |
-0.827 |
-0.897 |
0.441 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4347 | 0.9804 | 1.8803 |
O2 | 1.4347 | | 1.8803 | 0.9804 | H3 | 0.9804 | 1.8803 | | 2.4397 | H4 | 1.8803 | 0.9804 | 2.4397 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
100.566 |
|
O2 |
O1 |
H3 |
100.566 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.376 |
|
|
|
| 2 |
O |
-0.376 |
|
|
|
| 3 |
H |
0.376 |
|
|
|
| 4 |
H |
0.376 |
|
|
|
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 |
1.860 |
1.860 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.683 |
3.309 |
0.000 |
| y |
3.309 |
-11.822 |
0.000 |
| z |
0.000 |
0.000 |
-12.365 |
|
| Traceless |
| | x | y | z |
| x |
2.411 |
3.309 |
0.000 |
| y |
3.309 |
-0.798 |
0.000 |
| z |
0.000 |
0.000 |
-1.613 |
|
| Polar |
| 3z2-r2 | -3.226 |
| x2-y2 | 2.139 |
| xy | 3.309 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.727 |
0.213 |
0.000 |
| y |
0.213 |
2.329 |
0.000 |
| z |
0.000 |
0.000 |
1.603 |
<r2> (average value of r
2) Å
2
| <r2> |
18.698 |
| (<r2>)1/2 |
4.324 |
Jump to
S1C1
Energy calculated at LSDA/6-31+G**
| | hartrees |
| Energy at 0K | -150.828157 |
| Energy at 298.15K | |
| HF Energy | -150.828157 |
| Nuclear repulsion energy | 36.804911 |
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/6-31+G**
| 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 |
3709 |
3653 |
0.00 |
|
|
|
| 2 |
Ag |
1482 |
1460 |
0.00 |
|
|
|
| 3 |
Ag |
971 |
956 |
0.00 |
|
|
|
| 4 |
Au |
310i |
305i |
321.53 |
|
|
|
| 5 |
Bu |
3715 |
3660 |
118.46 |
|
|
|
| 6 |
Bu |
1197 |
1179 |
143.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5382.5 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 5301.8 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 LSDA/6-31+G**
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.723 |
0.000 |
| O2 |
0.000 |
-0.723 |
0.000 |
| H3 |
0.967 |
0.875 |
0.000 |
| H4 |
-0.967 |
-0.875 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4460 | 0.9789 | 1.8681 |
O2 | 1.4460 | | 1.8681 | 0.9789 | H3 | 0.9789 | 1.8681 | | 2.6086 | H4 | 1.8681 | 0.9789 | 2.6086 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
98.946 |
|
O2 |
O1 |
H3 |
98.946 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.382 |
|
|
|
| 2 |
O |
-0.382 |
|
|
|
| 3 |
H |
0.382 |
|
|
|
| 4 |
H |
0.382 |
|
|
|
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 |
-8.235 |
3.826 |
0.000 |
| y |
3.826 |
-11.956 |
0.000 |
| z |
0.000 |
0.000 |
-13.526 |
|
| Traceless |
| | x | y | z |
| x |
4.506 |
3.826 |
0.000 |
| y |
3.826 |
-1.076 |
0.000 |
| z |
0.000 |
0.000 |
-3.430 |
|
| Polar |
| 3z2-r2 | -6.860 |
| x2-y2 | 3.721 |
| xy | 3.826 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.792 |
0.224 |
0.000 |
| y |
0.224 |
2.341 |
0.000 |
| z |
0.000 |
0.000 |
1.517 |
<r2> (average value of r
2) Å
2
| <r2> |
18.786 |
| (<r2>)1/2 |
4.334 |