Jump to
S1C2
Vibrational Frequencies calculated at TPSSh/aug-cc-pVTZ
Geometric Data calculated at TPSSh/aug-cc-pVTZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at TPSSh/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -999.131275 |
| Energy at 298.15K | -999.136031 |
| HF Energy | -999.131275 |
| Nuclear repulsion energy | 201.436044 |
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 TPSSh/aug-cc-pVTZ
| 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 |
3131 |
3022 |
0.35 |
|
|
|
| 2 |
A |
3076 |
2969 |
22.94 |
|
|
|
| 3 |
A |
1476 |
1425 |
0.43 |
|
|
|
| 4 |
A |
1332 |
1285 |
15.29 |
|
|
|
| 5 |
A |
1217 |
1175 |
0.38 |
|
|
|
| 6 |
A |
1042 |
1005 |
1.46 |
|
|
|
| 7 |
A |
946 |
913 |
11.55 |
|
|
|
| 8 |
A |
654 |
631 |
19.11 |
|
|
|
| 9 |
A |
249 |
240 |
1.01 |
|
|
|
| 10 |
A |
107 |
103 |
0.83 |
|
|
|
| 11 |
B |
3145 |
3036 |
3.82 |
|
|
|
| 12 |
B |
3067 |
2960 |
2.89 |
|
|
|
| 13 |
B |
1474 |
1423 |
10.49 |
|
|
|
| 14 |
B |
1309 |
1264 |
41.07 |
|
|
|
| 15 |
B |
1154 |
1114 |
0.39 |
|
|
|
| 16 |
B |
889 |
858 |
17.99 |
|
|
|
| 17 |
B |
674 |
651 |
29.52 |
|
|
|
| 18 |
B |
397 |
383 |
8.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12669.8 cm
-1
Scaled (by 0.9652) Zero Point Vibrational Energy (zpe) 12228.9 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 TPSSh/aug-cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.298 |
0.694 |
0.899 |
| C2 |
-0.298 |
-0.694 |
0.899 |
| Cl3 |
-0.298 |
1.697 |
-0.472 |
| Cl4 |
0.298 |
-1.697 |
-0.472 |
| H5 |
0.005 |
1.214 |
1.810 |
| H6 |
1.382 |
0.666 |
0.821 |
| H7 |
-0.005 |
-1.214 |
1.810 |
| H8 |
-1.382 |
-0.666 |
0.821 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5099 | 1.8001 | 2.7559 | 1.0899 | 1.0872 | 2.1362 | 2.1626 |
C2 | 1.5099 | | 2.7559 | 1.8001 | 2.1362 | 2.1626 | 1.0899 | 1.0872 | Cl3 | 1.8001 | 2.7559 | | 3.4463 | 2.3524 | 2.3574 | 3.7110 | 2.9041 | Cl4 | 2.7559 | 1.8001 | 3.4463 | | 3.7110 | 2.9041 | 2.3524 | 2.3574 | H5 | 1.0899 | 2.1362 | 2.3524 | 3.7110 | | 1.7817 | 2.4285 | 2.5371 | H6 | 1.0872 | 2.1626 | 2.3574 | 2.9041 | 1.7817 | | 2.5371 | 3.0682 | H7 | 2.1362 | 1.0899 | 3.7110 | 2.3524 | 2.4285 | 2.5371 | | 1.7817 | H8 | 2.1626 | 1.0872 | 2.9041 | 2.3574 | 2.5371 | 3.0682 | 1.7817 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.439 |
|
C1 |
C2 |
H7 |
109.440 |
| C1 |
C2 |
H8 |
111.719 |
|
C2 |
C1 |
Cl3 |
112.439 |
| C2 |
C1 |
H5 |
109.440 |
|
C2 |
C1 |
H6 |
111.719 |
| Cl3 |
C1 |
H5 |
106.367 |
|
Cl3 |
C1 |
H6 |
106.860 |
| Cl4 |
C2 |
H7 |
106.367 |
|
Cl4 |
C2 |
H8 |
106.860 |
| H5 |
C1 |
H6 |
109.846 |
|
H7 |
C2 |
H8 |
109.846 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.017 |
|
|
|
| 2 |
C |
0.017 |
|
|
|
| 3 |
Cl |
-0.296 |
|
|
|
| 4 |
Cl |
-0.296 |
|
|
|
| 5 |
H |
0.116 |
|
|
|
| 6 |
H |
0.163 |
|
|
|
| 7 |
H |
0.116 |
|
|
|
| 8 |
H |
0.163 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.782 |
2.782 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.039 |
-0.456 |
0.000 |
| y |
-0.456 |
9.337 |
0.000 |
| z |
0.000 |
0.000 |
8.293 |
<r2> (average value of r
2) Å
2
| <r2> |
164.649 |
| (<r2>)1/2 |
12.832 |