Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-311G*
| | hartrees |
| Energy at 0K | -499.280200 |
| Energy at 298.15K | |
| HF Energy | -499.176465 |
| Nuclear repulsion energy | 45.232091 |
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/6-311G*
| 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' |
3203 |
3203 |
10.32 |
101.60 |
0.15 |
0.26 |
| 2 |
A' |
1448 |
1448 |
11.60 |
2.17 |
0.72 |
0.84 |
| 3 |
A' |
844 |
844 |
39.56 |
7.01 |
0.33 |
0.50 |
| 4 |
A' |
199 |
199 |
91.34 |
0.36 |
0.06 |
0.11 |
| 5 |
A" |
3358 |
3358 |
0.64 |
51.98 |
0.75 |
0.86 |
| 6 |
A" |
1029 |
1029 |
0.90 |
3.92 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5039.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5039.9 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 B2PLYP=FULL/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.007 |
1.123 |
0.000 |
| Cl2 |
-0.007 |
-0.587 |
0.000 |
| H3 |
0.082 |
1.618 |
0.952 |
| H4 |
0.082 |
1.618 |
-0.952 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7098 | 1.0765 | 1.0765 |
Cl2 | 1.7098 | | 2.4031 | 2.4031 | H3 | 1.0765 | 2.4031 | | 1.9034 | H4 | 1.0765 | 2.4031 | 1.9034 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.378 |
|
Br2 |
C1 |
H4 |
117.378 |
| H3 |
C1 |
H4 |
124.285 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-311G*
| | hartrees |
| Energy at 0K | -499.280191 |
| Energy at 298.15K | |
| HF Energy | -499.176433 |
| Nuclear repulsion energy | 45.244790 |
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/6-311G*
| 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 |
3206 |
3206 |
9.64 |
100.89 |
0.15 |
0.26 |
| 2 |
A1 |
1447 |
1447 |
11.81 |
|
|
|
| 3 |
A1 |
845 |
845 |
38.74 |
|
|
|
| 4 |
B1 |
141i |
141i |
97.37 |
|
|
|
| 5 |
B2 |
3363 |
3363 |
0.46 |
|
|
|
| 6 |
B2 |
1026 |
1026 |
0.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4872.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4872.7 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/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.122 |
| Cl2 |
0.000 |
0.000 |
0.587 |
| H3 |
0.000 |
0.953 |
-1.622 |
| H4 |
0.000 |
-0.953 |
-1.622 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7089 | 1.0761 | 1.0761 |
Cl2 | 1.7089 | | 2.4053 | 2.4053 | H3 | 1.0761 | 2.4053 | | 1.9064 | H4 | 1.0761 | 2.4053 | 1.9064 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.655 |
|
Br2 |
C1 |
H4 |
117.655 |
| H3 |
C1 |
H4 |
124.689 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability