Jump to
S1C2
Energy calculated at CISD/6-311G*
| | hartrees |
| Energy at 0K | -957.792891 |
| Energy at 298.15K | |
| HF Energy | -957.412558 |
| Nuclear repulsion energy | 125.748081 |
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 CISD/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 |
A1 |
3349 |
3098 |
0.13 |
|
|
|
| 2 |
A1 |
781 |
723 |
10.03 |
|
|
|
| 3 |
A1 |
327 |
302 |
0.32 |
|
|
|
| 4 |
B1 |
424i |
393i |
55.69 |
|
|
|
| 5 |
B2 |
1318 |
1219 |
57.24 |
|
|
|
| 6 |
B2 |
974 |
901 |
141.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3162.0 cm
-1
Scaled (by 0.9253) Zero Point Vibrational Energy (zpe) 2925.8 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 CISD/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.671 |
| H2 |
0.000 |
0.000 |
1.744 |
| Cl3 |
0.000 |
1.476 |
-0.170 |
| Cl4 |
0.000 |
-1.476 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0737 | 1.6987 | 1.6987 |
H2 | 1.0737 | | 2.4173 | 2.4173 | Cl3 | 1.6987 | 2.4173 | | 2.9525 | Cl4 | 1.6987 | 2.4173 | 2.9525 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.654 |
|
Cl3 |
C1 |
Cl4 |
120.693 |
| Cl4 |
C1 |
H2 |
119.654 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at CISD/6-311G*
| | hartrees |
| Energy at 0K | -957.793988 |
| Energy at 298.15K | -957.794872 |
| HF Energy | -957.414367 |
| Nuclear repulsion energy | 125.608478 |
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 CISD/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' |
3311 |
3063 |
2.77 |
|
|
|
| 2 |
A' |
789 |
730 |
16.05 |
|
|
|
| 3 |
A' |
547 |
507 |
24.68 |
|
|
|
| 4 |
A' |
321 |
297 |
0.49 |
|
|
|
| 5 |
A" |
1328 |
1229 |
49.06 |
|
|
|
| 6 |
A" |
943 |
873 |
167.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3619.8 cm
-1
Scaled (by 0.9253) Zero Point Vibrational Energy (zpe) 3349.4 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 CISD/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.695 |
0.000 |
| H2 |
-0.493 |
1.646 |
0.000 |
| Cl3 |
0.012 |
-0.171 |
1.472 |
| Cl4 |
0.012 |
-0.171 |
-1.472 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0770 | 1.7082 | 1.7082 |
H2 | 1.0770 | | 2.3929 | 2.3929 | Cl3 | 1.7082 | 2.3929 | | 2.9441 | Cl4 | 1.7082 | 2.3929 | 2.9441 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.610 |
|
Cl3 |
C1 |
Cl4 |
119.028 |
| Cl4 |
C1 |
H2 |
116.610 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability