Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -958.763150 |
| Energy at 298.15K | |
| HF Energy | -958.598388 |
| Nuclear repulsion energy | 125.400899 |
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 B2PLYP=FULLultrafine/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 |
3292 |
3292 |
0.15 |
|
|
|
| 2 |
A1 |
757 |
757 |
8.56 |
|
|
|
| 3 |
A1 |
319 |
319 |
0.17 |
|
|
|
| 4 |
B1 |
392i |
392i |
62.27 |
|
|
|
| 5 |
B2 |
1279 |
1279 |
50.32 |
|
|
|
| 6 |
B2 |
925 |
925 |
170.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3090.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3090.2 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 B2PLYP=FULLultrafine/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 |
1.747 |
| Cl3 |
0.000 |
1.481 |
-0.170 |
| Cl4 |
0.000 |
-1.481 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0756 | 1.7030 | 1.7030 |
H2 | 1.0756 | | 2.4220 | 2.4220 | Cl3 | 1.7030 | 2.4220 | | 2.9620 | Cl4 | 1.7030 | 2.4220 | 2.9620 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.586 |
|
Cl3 |
C1 |
Cl4 |
120.828 |
| Cl4 |
C1 |
H2 |
119.586 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -958.764117 |
| Energy at 298.15K | |
| HF Energy | -958.599455 |
| Nuclear repulsion energy | 125.193243 |
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 B2PLYP=FULLultrafine/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' |
3253 |
3253 |
2.96 |
|
|
|
| 2 |
A' |
766 |
766 |
15.30 |
|
|
|
| 3 |
A' |
512 |
512 |
30.16 |
|
|
|
| 4 |
A' |
313 |
313 |
0.48 |
|
|
|
| 5 |
A" |
1288 |
1288 |
42.31 |
|
|
|
| 6 |
A" |
891 |
891 |
199.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3511.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3511.0 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 B2PLYP=FULLultrafine/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.696 |
0.000 |
| H2 |
-0.495 |
1.648 |
0.000 |
| Cl3 |
0.012 |
-0.171 |
1.478 |
| Cl4 |
0.012 |
-0.171 |
-1.478 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0788 | 1.7134 | 1.7134 |
H2 | 1.0788 | | 2.3981 | 2.3981 | Cl3 | 1.7134 | 2.3981 | | 2.9555 | Cl4 | 1.7134 | 2.3981 | 2.9555 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.528 |
|
Cl3 |
C1 |
Cl4 |
119.188 |
| Cl4 |
C1 |
H2 |
116.528 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability