Jump to
S1C2
Energy calculated at MP2=FULL/6-311G*
| | hartrees |
| Energy at 0K | -957.921304 |
| Energy at 298.15K | |
| HF Energy | -957.412423 |
| Nuclear repulsion energy | 126.102102 |
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=FULL/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 |
3325 |
3149 |
0.01 |
|
|
|
| 2 |
A1 |
785 |
744 |
9.22 |
|
|
|
| 3 |
A1 |
329 |
312 |
0.18 |
|
|
|
| 4 |
B1 |
440i |
416i |
63.16 |
|
|
|
| 5 |
B2 |
1308 |
1238 |
51.67 |
|
|
|
| 6 |
B2 |
971 |
920 |
160.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3138.9 cm
-1
Scaled (by 0.9471) Zero Point Vibrational Energy (zpe) 2972.8 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 MP2=FULL/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.668 |
| H2 |
0.000 |
0.000 |
1.744 |
| Cl3 |
0.000 |
1.472 |
-0.169 |
| Cl4 |
0.000 |
-1.472 |
-0.169 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0761 | 1.6934 | 1.6934 |
H2 | 1.0761 | | 2.4140 | 2.4140 | Cl3 | 1.6934 | 2.4140 | | 2.9439 | Cl4 | 1.6934 | 2.4140 | 2.9439 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.631 |
|
Cl3 |
C1 |
Cl4 |
120.738 |
| Cl4 |
C1 |
H2 |
119.631 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2=FULL/6-311G*
| | hartrees |
| Energy at 0K | -957.922522 |
| Energy at 298.15K | -957.923413 |
| HF Energy | -957.414262 |
| Nuclear repulsion energy | 125.892342 |
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=FULL/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' |
3277 |
3104 |
2.69 |
|
|
|
| 2 |
A' |
793 |
751 |
16.21 |
|
|
|
| 3 |
A' |
555 |
526 |
27.57 |
|
|
|
| 4 |
A' |
323 |
306 |
0.36 |
|
|
|
| 5 |
A" |
1317 |
1247 |
44.30 |
|
|
|
| 6 |
A" |
936 |
886 |
188.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3600.5 cm
-1
Scaled (by 0.9471) Zero Point Vibrational Energy (zpe) 3410.1 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=FULL/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.693 |
0.000 |
| H2 |
-0.503 |
1.642 |
0.000 |
| Cl3 |
0.013 |
-0.171 |
1.469 |
| Cl4 |
0.013 |
-0.171 |
-1.469 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0801 | 1.7039 | 1.7039 |
H2 | 1.0801 | | 2.3895 | 2.3895 | Cl3 | 1.7039 | 2.3895 | | 2.9373 | Cl4 | 1.7039 | 2.3895 | 2.9373 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.455 |
|
Cl3 |
C1 |
Cl4 |
119.071 |
| Cl4 |
C1 |
H2 |
116.455 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability