Jump to
S1C2
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -150.849106 |
| Energy at 298.15K | -150.851378 |
| HF Energy | -150.849106 |
| Nuclear repulsion energy | 37.023006 |
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/6-311G*
| 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 |
3628 |
3569 |
4.55 |
|
|
|
| 2 |
A |
1457 |
1433 |
0.30 |
|
|
|
| 3 |
A |
963 |
948 |
2.61 |
|
|
|
| 4 |
A |
357 |
351 |
248.14 |
|
|
|
| 5 |
B |
3630 |
3571 |
30.15 |
|
|
|
| 6 |
B |
1291 |
1270 |
110.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5663.2 cm
-1
Scaled (by 0.9837) Zero Point Vibrational Energy (zpe) 5570.9 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/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.716 |
-0.053 |
| O2 |
0.000 |
-0.716 |
-0.053 |
| H3 |
0.834 |
0.898 |
0.422 |
| H4 |
-0.834 |
-0.898 |
0.422 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4330 | 0.9770 | 1.8787 |
O2 | 1.4330 | | 1.8787 | 0.9770 | H3 | 0.9770 | 1.8787 | | 2.4518 | H4 | 1.8787 | 0.9770 | 2.4518 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
100.734 |
|
O2 |
O1 |
H3 |
100.734 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.423 |
|
|
|
| 2 |
O |
-0.423 |
|
|
|
| 3 |
H |
0.423 |
|
|
|
| 4 |
H |
0.423 |
|
|
|
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 |
1.907 |
1.907 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.225 |
3.347 |
0.000 |
| y |
3.347 |
-11.392 |
0.000 |
| z |
0.000 |
0.000 |
-11.913 |
|
| Traceless |
| | x | y | z |
| x |
2.427 |
3.347 |
0.000 |
| y |
3.347 |
-0.822 |
0.000 |
| z |
0.000 |
0.000 |
-1.605 |
|
| Polar |
| 3z2-r2 | -3.210 |
| x2-y2 | 2.167 |
| xy | 3.347 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.416 |
0.328 |
0.000 |
| y |
0.328 |
1.943 |
0.000 |
| z |
0.000 |
0.000 |
0.938 |
<r2> (average value of r
2) Å
2
| <r2> |
18.393 |
| (<r2>)1/2 |
4.289 |
Jump to
S1C1
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -150.848072 |
| Energy at 298.15K | |
| HF Energy | -150.848072 |
| Nuclear repulsion energy | 36.850676 |
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/6-311G*
| 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 |
3672 |
3612 |
0.00 |
|
|
|
| 2 |
Ag |
1543 |
1518 |
0.00 |
|
|
|
| 3 |
Ag |
966 |
950 |
0.00 |
|
|
|
| 4 |
Au |
255i |
251i |
370.56 |
|
|
|
| 5 |
Bu |
3684 |
3624 |
69.00 |
|
|
|
| 6 |
Bu |
1227 |
1207 |
152.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5417.9 cm
-1
Scaled (by 0.9837) Zero Point Vibrational Energy (zpe) 5329.6 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/6-311G*
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 |
0.963 |
0.876 |
0.000 |
| H4 |
-0.963 |
-0.876 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4455 | 0.9753 | 1.8662 |
O2 | 1.4455 | | 1.8662 | 0.9753 | H3 | 0.9753 | 1.8662 | | 2.6035 | H4 | 1.8662 | 0.9753 | 2.6035 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
99.019 |
|
O2 |
O1 |
H3 |
99.019 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.429 |
|
|
|
| 2 |
O |
-0.429 |
|
|
|
| 3 |
H |
0.429 |
|
|
|
| 4 |
H |
0.429 |
|
|
|
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 |
-7.933 |
3.841 |
0.000 |
| y |
3.841 |
-11.534 |
0.000 |
| z |
0.000 |
0.000 |
-12.910 |
|
| Traceless |
| | x | y | z |
| x |
4.288 |
3.841 |
0.000 |
| y |
3.841 |
-1.112 |
0.000 |
| z |
0.000 |
0.000 |
-3.176 |
|
| Polar |
| 3z2-r2 | -6.353 |
| x2-y2 | 3.600 |
| xy | 3.841 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.626 |
0.331 |
0.000 |
| y |
0.331 |
1.949 |
0.000 |
| z |
0.000 |
0.000 |
0.712 |
<r2> (average value of r
2) Å
2
| <r2> |
18.488 |
| (<r2>)1/2 |
4.300 |