Jump to
S1C2
Energy calculated at B2PLYP=FULL/cc-pVDZ
| | hartrees |
| Energy at 0K | -958.718177 |
| Energy at 298.15K | |
| HF Energy | -958.584768 |
| Nuclear repulsion energy | 124.970697 |
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/cc-pVDZ
| 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 |
3290 |
3153 |
0.24 |
|
|
|
| 2 |
A1 |
757 |
725 |
10.52 |
|
|
|
| 3 |
A1 |
310 |
297 |
0.39 |
|
|
|
| 4 |
B1 |
421i |
404i |
49.97 |
|
|
|
| 5 |
B2 |
1228 |
1177 |
54.25 |
|
|
|
| 6 |
B2 |
930 |
891 |
151.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3046.2 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 2919.8 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 B2PLYP=FULL/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.676 |
| H2 |
0.000 |
0.000 |
1.762 |
| Cl3 |
0.000 |
1.485 |
-0.171 |
| Cl4 |
0.000 |
-1.485 |
-0.171 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0863 | 1.7092 | 1.7092 |
H2 | 1.0863 | | 2.4376 | 2.4376 | Cl3 | 1.7092 | 2.4376 | | 2.9691 | Cl4 | 1.7092 | 2.4376 | 2.9691 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.707 |
|
Cl3 |
C1 |
Cl4 |
120.587 |
| Cl4 |
C1 |
H2 |
119.707 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/cc-pVDZ
| | hartrees |
| Energy at 0K | -958.719446 |
| Energy at 298.15K | -958.720280 |
| HF Energy | -958.586042 |
| Nuclear repulsion energy | 124.774647 |
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/cc-pVDZ
| 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' |
3241 |
3107 |
1.89 |
|
|
|
| 2 |
A' |
764 |
733 |
17.10 |
|
|
|
| 3 |
A' |
536 |
514 |
21.51 |
|
|
|
| 4 |
A' |
305 |
292 |
0.39 |
|
|
|
| 5 |
A" |
1232 |
1181 |
42.40 |
|
|
|
| 6 |
A" |
892 |
855 |
181.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3484.8 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 3340.1 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 B2PLYP=FULL/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.704 |
0.000 |
| H2 |
-0.528 |
1.651 |
0.000 |
| Cl3 |
0.013 |
-0.173 |
1.480 |
| Cl4 |
0.013 |
-0.173 |
-1.480 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0904 | 1.7206 | 1.7206 |
H2 | 1.0904 | | 2.4105 | 2.4105 | Cl3 | 1.7206 | 2.4105 | | 2.9604 | Cl4 | 1.7206 | 2.4105 | 2.9604 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.278 |
|
Cl3 |
C1 |
Cl4 |
118.690 |
| Cl4 |
C1 |
H2 |
116.278 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability