Jump to
S1C2
Energy calculated at MP2/LANL2DZ
| hartrees |
Energy at 0K | -151.006550 |
Energy at 298.15K | -151.008305 |
HF Energy | -150.747622 |
Nuclear repulsion energy | 34.767170 |
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 MP2/LANL2DZ
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 |
3591 |
3458 |
0.00 |
126.35 |
0.40 |
0.57 |
2 |
A |
1435 |
1382 |
0.00 |
12.88 |
0.69 |
0.82 |
3 |
A |
810 |
780 |
0.00 |
2.56 |
0.22 |
0.36 |
4 |
A |
47 |
45 |
457.48 |
0.00 |
0.73 |
0.84 |
5 |
B |
3605 |
3472 |
34.55 |
0.00 |
0.75 |
0.86 |
6 |
B |
1125 |
1084 |
187.45 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5306.3 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 5110.5 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 MP2/LANL2DZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.780 |
0.000 |
O2 |
0.000 |
-0.780 |
0.000 |
H3 |
0.984 |
0.910 |
-0.000 |
H4 |
-0.984 |
-0.910 |
-0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.5602 | 0.9922 | 1.9554 |
O2 | 1.5602 | | 1.9554 | 0.9922 | H3 | 0.9922 | 1.9554 | | 2.6799 | H4 | 1.9554 | 0.9922 | 2.6799 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
97.511 |
|
O2 |
O1 |
H3 |
97.511 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2/LANL2DZ
| hartrees |
Energy at 0K | -151.006550 |
Energy at 298.15K | -151.008319 |
HF Energy | -150.747616 |
Nuclear repulsion energy | 34.767059 |
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 MP2/LANL2DZ
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 |
3457 |
0.00 |
|
|
|
2 |
Ag |
1435 |
1382 |
0.00 |
|
|
|
3 |
Ag |
810 |
780 |
0.00 |
|
|
|
4 |
Au |
54 |
52 |
457.43 |
|
|
|
5 |
Bu |
3604 |
3471 |
34.53 |
|
|
|
6 |
Bu |
1125 |
1084 |
187.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5309.4 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 5113.5 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 MP2/LANL2DZ
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.780 |
0.000 |
O2 |
0.000 |
-0.780 |
0.000 |
H3 |
0.984 |
0.910 |
0.000 |
H4 |
-0.984 |
-0.910 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.5602 | 0.9923 | 1.9554 |
O2 | 1.5602 | | 1.9554 | 0.9923 | H3 | 0.9923 | 1.9554 | | 2.6799 | H4 | 1.9554 | 0.9923 | 2.6799 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
97.508 |
|
O2 |
O1 |
H3 |
97.508 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability