Jump to
S1C2
Energy calculated at MP2=FULL/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -498.811282 |
| Energy at 298.15K | |
| HF Energy | -498.471824 |
| Nuclear repulsion energy | 45.617748 |
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/6-31G(2df,p)
| 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' |
3268 |
3072 |
5.58 |
|
|
|
| 2 |
A' |
1451 |
1364 |
12.00 |
|
|
|
| 3 |
A' |
883 |
830 |
36.82 |
|
|
|
| 4 |
A' |
335 |
315 |
58.64 |
|
|
|
| 5 |
A" |
3424 |
3218 |
0.71 |
|
|
|
| 6 |
A" |
1030 |
968 |
0.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5195.3 cm
-1
Scaled (by 0.9399) Zero Point Vibrational Energy (zpe) 4883.1 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/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.011 |
1.112 |
0.000 |
| Cl2 |
-0.011 |
-0.581 |
0.000 |
| H3 |
0.131 |
1.604 |
0.944 |
| H4 |
0.131 |
1.604 |
-0.944 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.6929 | 1.0745 | 1.0745 |
Cl2 | 1.6929 | | 2.3850 | 2.3850 | H3 | 1.0745 | 2.3850 | | 1.8885 | H4 | 1.0745 | 2.3850 | 1.8885 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.288 |
|
Br2 |
C1 |
H4 |
117.288 |
| H3 |
C1 |
H4 |
123.005 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2=FULL/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -498.811221 |
| Energy at 298.15K | |
| HF Energy | -498.471609 |
| Nuclear repulsion energy | 45.660603 |
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/6-31G(2df,p)
| 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 |
3279 |
3082 |
3.95 |
|
|
|
| 2 |
A1 |
1450 |
1362 |
12.33 |
|
|
|
| 3 |
A1 |
886 |
833 |
35.02 |
|
|
|
| 4 |
B1 |
243i |
228i |
69.00 |
|
|
|
| 5 |
B2 |
3438 |
3232 |
1.41 |
|
|
|
| 6 |
B2 |
1023 |
962 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4916.7 cm
-1
Scaled (by 0.9399) Zero Point Vibrational Energy (zpe) 4621.2 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 MP2=FULL/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.109 |
| Cl2 |
0.000 |
0.000 |
0.581 |
| H3 |
0.000 |
0.948 |
-1.612 |
| H4 |
0.000 |
-0.948 |
-1.612 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.6902 | 1.0733 | 1.0733 |
Cl2 | 1.6902 | | 2.3892 | 2.3892 | H3 | 1.0733 | 2.3892 | | 1.8966 | H4 | 1.0733 | 2.3892 | 1.8966 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.929 |
|
Br2 |
C1 |
H4 |
117.929 |
| H3 |
C1 |
H4 |
124.142 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability