Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-311G**
| | hartrees |
| Energy at 0K | -958.766966 |
| Energy at 298.15K | |
| HF Energy | -958.600407 |
| Nuclear repulsion energy | 125.434076 |
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=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 |
3296 |
3296 |
0.00 |
|
|
|
| 2 |
A1 |
758 |
758 |
8.44 |
|
|
|
| 3 |
A1 |
318 |
318 |
0.16 |
|
|
|
| 4 |
B1 |
378i |
378i |
58.83 |
|
|
|
| 5 |
B2 |
1273 |
1273 |
51.21 |
|
|
|
| 6 |
B2 |
925 |
925 |
171.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3096.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3096.2 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=FULL/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.672 |
| H2 |
0.000 |
0.000 |
1.747 |
| Cl3 |
0.000 |
1.480 |
-0.170 |
| Cl4 |
0.000 |
-1.480 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0750 | 1.7029 | 1.7029 |
H2 | 1.0750 | | 2.4217 | 2.4217 | Cl3 | 1.7029 | 2.4217 | | 2.9606 | Cl4 | 1.7029 | 2.4217 | 2.9606 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.623 |
|
Cl3 |
C1 |
Cl4 |
120.754 |
| Cl4 |
C1 |
H2 |
119.623 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-311G**
| | hartrees |
| Energy at 0K | -958.767822 |
| Energy at 298.15K | -958.768642 |
| HF Energy | -958.601335 |
| Nuclear repulsion energy | 125.228642 |
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=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' |
3258 |
3258 |
2.02 |
|
|
|
| 2 |
A' |
765 |
765 |
14.36 |
|
|
|
| 3 |
A' |
497 |
497 |
29.90 |
|
|
|
| 4 |
A' |
313 |
313 |
0.51 |
|
|
|
| 5 |
A" |
1279 |
1279 |
43.63 |
|
|
|
| 6 |
A" |
892 |
892 |
198.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3501.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3501.4 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 B2PLYP=FULL/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.695 |
0.000 |
| H2 |
-0.483 |
1.653 |
0.000 |
| Cl3 |
0.012 |
-0.171 |
1.477 |
| Cl4 |
0.012 |
-0.171 |
-1.477 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0782 | 1.7127 | 1.7127 |
H2 | 1.0782 | | 2.3991 | 2.3991 | Cl3 | 1.7127 | 2.3991 | | 2.9549 | Cl4 | 1.7127 | 2.3991 | 2.9549 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.707 |
|
Cl3 |
C1 |
Cl4 |
119.226 |
| Cl4 |
C1 |
H2 |
116.707 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability