Jump to
S1C2
Energy calculated at CID/6-311G*
| | hartrees |
| Energy at 0K | -498.751728 |
| Energy at 298.15K | |
| HF Energy | -498.492976 |
| Nuclear repulsion energy | 45.262040 |
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 CID/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' |
3239 |
3009 |
9.76 |
|
|
|
| 2 |
A' |
1478 |
1373 |
12.25 |
|
|
|
| 3 |
A' |
868 |
806 |
38.09 |
|
|
|
| 4 |
A' |
282 |
262 |
80.35 |
|
|
|
| 5 |
A" |
3390 |
3150 |
0.57 |
|
|
|
| 6 |
A" |
1049 |
974 |
0.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5151.9 cm
-1
Scaled (by 0.9291) Zero Point Vibrational Energy (zpe) 4786.6 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 CID/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.009 |
1.122 |
0.000 |
| Cl2 |
-0.009 |
-0.586 |
0.000 |
| H3 |
0.109 |
1.617 |
0.949 |
| H4 |
0.109 |
1.617 |
-0.949 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7084 | 1.0767 | 1.0767 |
Cl2 | 1.7084 | | 2.4017 | 2.4017 | H3 | 1.0767 | 2.4017 | | 1.8979 | H4 | 1.0767 | 2.4017 | 1.8979 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.352 |
|
Br2 |
C1 |
H4 |
117.352 |
| H3 |
C1 |
H4 |
123.618 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at CID/6-311G*
| | hartrees |
| Energy at 0K | -498.751698 |
| Energy at 298.15K | |
| HF Energy | -498.492790 |
| Nuclear repulsion energy | 45.284893 |
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 CID/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 |
3245 |
3015 |
8.64 |
|
|
|
| 2 |
A1 |
1476 |
1371 |
12.57 |
|
|
|
| 3 |
A1 |
870 |
808 |
36.87 |
|
|
|
| 4 |
B1 |
203i |
188i |
91.02 |
|
|
|
| 5 |
B2 |
3400 |
3159 |
0.28 |
|
|
|
| 6 |
B2 |
1043 |
969 |
0.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4916.1 cm
-1
Scaled (by 0.9291) Zero Point Vibrational Energy (zpe) 4567.5 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 CID/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.121 |
| Cl2 |
0.000 |
0.000 |
0.586 |
| H3 |
0.000 |
0.952 |
-1.622 |
| H4 |
0.000 |
-0.952 |
-1.622 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7068 | 1.0759 | 1.0759 |
Cl2 | 1.7068 | | 2.4049 | 2.4049 | H3 | 1.0759 | 2.4049 | | 1.9034 | H4 | 1.0759 | 2.4049 | 1.9034 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.800 |
|
Br2 |
C1 |
H4 |
117.800 |
| H3 |
C1 |
H4 |
124.400 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability