Jump to
S1C2
Energy calculated at MP3=FULL/6-311G*
| | hartrees |
| Energy at 0K | -498.836655 |
| Energy at 298.15K | |
| HF Energy | -498.492887 |
| Nuclear repulsion energy | 45.267882 |
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 MP3=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' |
3225 |
3225 |
8.66 |
|
|
|
| 2 |
A' |
1467 |
1467 |
10.61 |
|
|
|
| 3 |
A' |
866 |
866 |
36.63 |
|
|
|
| 4 |
A' |
226 |
226 |
87.36 |
|
|
|
| 5 |
A" |
3377 |
3377 |
0.27 |
|
|
|
| 6 |
A" |
1041 |
1041 |
0.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5100.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5100.9 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 MP3=FULL/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.008 |
1.121 |
0.000 |
| Cl2 |
-0.008 |
-0.586 |
0.000 |
| H3 |
0.089 |
1.619 |
0.951 |
| H4 |
0.089 |
1.619 |
-0.951 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7075 | 1.0777 | 1.0777 |
Cl2 | 1.7075 | | 2.4033 | 2.4033 | H3 | 1.0777 | 2.4033 | | 1.9024 | H4 | 1.0777 | 2.4033 | 1.9024 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.485 |
|
Br2 |
C1 |
H4 |
117.485 |
| H3 |
C1 |
H4 |
123.907 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP3=FULL/6-311G*
| | hartrees |
| Energy at 0K | -498.836641 |
| Energy at 298.15K | |
| HF Energy | -498.492751 |
| Nuclear repulsion energy | 45.283449 |
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 MP3=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 |
3229 |
3229 |
7.94 |
|
|
|
| 2 |
A1 |
1467 |
1467 |
10.81 |
|
|
|
| 3 |
A1 |
868 |
868 |
35.81 |
|
|
|
| 4 |
B1 |
163i |
163i |
94.76 |
|
|
|
| 5 |
B2 |
3383 |
3383 |
0.14 |
|
|
|
| 6 |
B2 |
1038 |
1038 |
0.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4910.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4910.7 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 MP3=FULL/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.120 |
| Cl2 |
0.000 |
0.000 |
0.586 |
| H3 |
0.000 |
0.953 |
-1.623 |
| H4 |
0.000 |
-0.953 |
-1.623 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7063 | 1.0773 | 1.0773 |
Cl2 | 1.7063 | | 2.4057 | 2.4057 | H3 | 1.0773 | 2.4057 | | 1.9058 | H4 | 1.0773 | 2.4057 | 1.9058 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.809 |
|
Br2 |
C1 |
H4 |
117.809 |
| H3 |
C1 |
H4 |
124.383 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability