Jump to
S1C2
Energy calculated at B3PW91/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -151.550898 |
Energy at 298.15K | -151.553238 |
HF Energy | -151.550898 |
Nuclear repulsion energy | 37.176985 |
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 B3PW91/6-311+G(3df,2p)
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 |
3807 |
3644 |
15.26 |
89.56 |
0.12 |
0.21 |
2 |
A |
1456 |
1394 |
0.32 |
6.56 |
0.36 |
0.53 |
3 |
A |
982 |
940 |
0.66 |
13.80 |
0.23 |
0.37 |
4 |
A |
414 |
396 |
164.90 |
0.88 |
0.73 |
0.85 |
5 |
B |
3806 |
3644 |
53.46 |
29.17 |
0.75 |
0.86 |
6 |
B |
1355 |
1297 |
97.99 |
1.38 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5910.3 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 5657.9 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 B3PW91/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.716 |
-0.060 |
O2 |
0.000 |
-0.716 |
-0.060 |
H3 |
0.777 |
0.901 |
0.480 |
H4 |
-0.777 |
-0.901 |
0.480 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4317 | 0.9642 | 1.8735 |
O2 | 1.4317 | | 1.8735 | 0.9642 | H3 | 0.9642 | 1.8735 | | 2.3797 | H4 | 1.8735 | 0.9642 | 2.3797 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
101.075 |
|
O2 |
O1 |
H3 |
101.075 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.241 |
|
|
|
2 |
O |
-0.241 |
|
|
|
3 |
H |
0.241 |
|
|
|
4 |
H |
0.241 |
|
|
|
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 |
1.817 |
1.817 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-9.879 |
2.896 |
0.000 |
y |
2.896 |
-11.391 |
0.000 |
z |
0.000 |
0.000 |
-11.798 |
|
Traceless |
| x | y | z |
x |
1.715 |
2.896 |
0.000 |
y |
2.896 |
-0.552 |
0.000 |
z |
0.000 |
0.000 |
-1.163 |
|
Polar |
3z2-r2 | -2.327 |
x2-y2 | 1.511 |
xy | 2.896 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.877 |
0.227 |
0.000 |
y |
0.227 |
2.577 |
0.000 |
z |
0.000 |
0.000 |
1.751 |
<r2> (average value of r
2) Å
2
<r2> |
18.434 |
(<r2>)1/2 |
4.294 |
Jump to
S1C1
Energy calculated at B3PW91/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -151.548853 |
Energy at 298.15K | |
HF Energy | -151.548853 |
Nuclear repulsion energy | 37.022762 |
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 B3PW91/6-311+G(3df,2p)
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 |
3846 |
3682 |
0.00 |
|
|
|
2 |
Ag |
1559 |
1492 |
0.00 |
|
|
|
3 |
Ag |
984 |
942 |
0.00 |
|
|
|
4 |
Au |
316i |
303i |
259.88 |
|
|
|
5 |
Bu |
3855 |
3690 |
108.94 |
|
|
|
6 |
Bu |
1262 |
1208 |
131.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5594.8 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 5355.9 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 B3PW91/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.721 |
0.000 |
O2 |
0.000 |
-0.721 |
0.000 |
H3 |
0.950 |
0.879 |
0.000 |
H4 |
-0.950 |
-0.879 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4429 | 0.9626 | 1.8608 |
O2 | 1.4429 | | 1.8608 | 0.9626 | H3 | 0.9626 | 1.8608 | | 2.5877 | H4 | 1.8608 | 0.9626 | 2.5877 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
99.412 |
|
O2 |
O1 |
H3 |
99.412 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.248 |
|
|
|
2 |
O |
-0.248 |
|
|
|
3 |
H |
0.248 |
|
|
|
4 |
H |
0.248 |
|
|
|
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 |
-8.239 |
3.486 |
0.000 |
y |
3.486 |
-11.527 |
0.000 |
z |
0.000 |
0.000 |
-13.136 |
|
Traceless |
| x | y | z |
x |
4.093 |
3.486 |
0.000 |
y |
3.486 |
-0.840 |
0.000 |
z |
0.000 |
0.000 |
-3.253 |
|
Polar |
3z2-r2 | -6.506 |
x2-y2 | 3.288 |
xy | 3.486 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.970 |
0.248 |
0.000 |
y |
0.248 |
2.582 |
0.000 |
z |
0.000 |
0.000 |
1.654 |
<r2> (average value of r
2) Å
2
<r2> |
18.526 |
(<r2>)1/2 |
4.304 |