Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-31+G**
| | hartrees |
| Energy at 0K | -958.677329 |
| Energy at 298.15K | |
| HF Energy | -958.543349 |
| Nuclear repulsion energy | 125.413273 |
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/6-31+G**
| 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 |
3320 |
3157 |
0.38 |
|
|
|
| 2 |
A1 |
763 |
726 |
8.58 |
|
|
|
| 3 |
A1 |
317 |
302 |
0.31 |
|
|
|
| 4 |
B1 |
380i |
362i |
57.02 |
|
|
|
| 5 |
B2 |
1279 |
1216 |
56.42 |
|
|
|
| 6 |
B2 |
936 |
890 |
163.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3117.0 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 2964.3 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/6-31+G**
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 | | 1.0760 | 1.7028 | 1.7028 |
H2 | 1.0760 | | 2.4220 | 2.4220 | Cl3 | 1.7028 | 2.4220 | | 2.9617 | Cl4 | 1.7028 | 2.4220 | 2.9617 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.581 |
|
Cl3 |
C1 |
Cl4 |
120.837 |
| Cl4 |
C1 |
H2 |
119.581 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-31+G**
| | hartrees |
| Energy at 0K | -958.678157 |
| Energy at 298.15K | -958.678974 |
| HF Energy | -958.544184 |
| Nuclear repulsion energy | 125.241411 |
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/6-31+G**
| 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' |
3279 |
3118 |
1.04 |
|
|
|
| 2 |
A' |
770 |
732 |
14.20 |
|
|
|
| 3 |
A' |
498 |
473 |
26.86 |
|
|
|
| 4 |
A' |
311 |
296 |
0.55 |
|
|
|
| 5 |
A" |
1284 |
1221 |
48.43 |
|
|
|
| 6 |
A" |
904 |
859 |
189.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3522.3 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 3349.7 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/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.694 |
0.000 |
| H2 |
-0.476 |
1.657 |
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 | | 1.0793 | 1.7121 | 1.7121 |
H2 | 1.0793 | | 2.4005 | 2.4005 | Cl3 | 1.7121 | 2.4005 | | 2.9550 | Cl4 | 1.7121 | 2.4005 | 2.9550 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.794 |
|
Cl3 |
C1 |
Cl4 |
119.301 |
| Cl4 |
C1 |
H2 |
116.794 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability