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S1C2
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -1072.683789 |
| Energy at 298.15K | |
| Nuclear repulsion energy | |
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=FULLultrafine/6-311G*
Geometric Data calculated at B2PLYP=FULLultrafine/6-311G*
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -1072.680776 |
| Energy at 298.15K | |
| HF Energy | -1072.389611 |
| Nuclear repulsion energy | 265.429540 |
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=FULLultrafine/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 |
3144 |
3144 |
5.97 |
79.73 |
0.22 |
0.36 |
| 2 |
A |
2982 |
2982 |
64.19 |
146.78 |
0.32 |
0.49 |
| 3 |
A |
1823 |
1823 |
128.74 |
13.28 |
0.56 |
0.72 |
| 4 |
A |
1420 |
1420 |
15.75 |
4.25 |
0.52 |
0.68 |
| 5 |
A |
1296 |
1296 |
18.93 |
4.89 |
0.69 |
0.81 |
| 6 |
A |
1262 |
1262 |
10.68 |
8.36 |
0.75 |
0.86 |
| 7 |
A |
1038 |
1038 |
15.69 |
2.41 |
0.49 |
0.65 |
| 8 |
A |
942 |
942 |
10.67 |
5.64 |
0.64 |
0.78 |
| 9 |
A |
812 |
812 |
84.62 |
7.16 |
0.73 |
0.84 |
| 10 |
A |
647 |
647 |
37.07 |
9.25 |
0.09 |
0.17 |
| 11 |
A |
620 |
620 |
40.09 |
7.83 |
0.46 |
0.63 |
| 12 |
A |
347 |
347 |
1.94 |
3.20 |
0.25 |
0.40 |
| 13 |
A |
281 |
281 |
2.77 |
6.25 |
0.65 |
0.79 |
| 14 |
A |
224 |
224 |
2.46 |
1.79 |
0.71 |
0.83 |
| 15 |
A |
88 |
88 |
10.33 |
2.30 |
0.73 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 8462.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8462.5 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 B2PLYP=FULLultrafine/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.098 |
-0.022 |
0.520 |
| C2 |
-0.712 |
-1.285 |
0.200 |
| H3 |
0.229 |
0.063 |
1.597 |
| Cl4 |
1.740 |
-0.256 |
-0.169 |
| Cl5 |
-0.683 |
1.451 |
-0.058 |
| O6 |
-1.790 |
-1.292 |
-0.322 |
| H7 |
-0.194 |
-2.210 |
0.512 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5338 | 1.0884 | 1.7963 | 1.7650 | 2.4258 | 2.2067 |
C2 | 1.5338 | | 2.1576 | 2.6853 | 2.7483 | 1.1974 | 1.1055 | H3 | 1.0884 | 2.1576 | | 2.3464 | 2.3443 | 3.0976 | 2.5539 | Cl4 | 1.7963 | 2.6853 | 2.3464 | | 2.9663 | 3.6823 | 2.8325 | Cl5 | 1.7650 | 2.7483 | 2.3443 | 2.9663 | | 2.9698 | 3.7373 | O6 | 2.4258 | 1.1974 | 3.0976 | 3.6823 | 2.9698 | | 2.0216 | H7 | 2.2067 | 1.1055 | 2.5539 | 2.8325 | 3.7373 | 2.0216 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
124.832 |
|
C1 |
C2 |
H7 |
112.445 |
| C2 |
C1 |
H3 |
109.565 |
|
C2 |
C1 |
Cl4 |
107.224 |
| C2 |
C1 |
Cl5 |
112.655 |
|
H3 |
C1 |
Cl4 |
106.251 |
| H3 |
C1 |
Cl5 |
108.133 |
|
Cl4 |
C1 |
Cl5 |
112.799 |
| O6 |
C2 |
H7 |
122.722 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.457 |
|
|
|
| 2 |
C |
0.145 |
|
|
|
| 3 |
H |
0.313 |
|
|
|
| 4 |
Cl |
-0.006 |
|
|
|
| 5 |
Cl |
0.023 |
|
|
|
| 6 |
O |
-0.222 |
|
|
|
| 7 |
H |
0.204 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.085 |
-0.902 |
1.995 |
2.443 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.316 |
-1.984 |
-1.212 |
| y |
-1.984 |
-42.414 |
-1.554 |
| z |
-1.212 |
-1.554 |
-40.968 |
|
| Traceless |
| | x | y | z |
| x |
-6.625 |
-1.984 |
-1.212 |
| y |
-1.984 |
2.228 |
-1.554 |
| z |
-1.212 |
-1.554 |
4.397 |
|
| Polar |
| 3z2-r2 | 8.795 |
| x2-y2 | -5.902 |
| xy | -1.984 |
| xz | -1.212 |
| yz | -1.554 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.988 |
-0.878 |
0.135 |
| y |
-0.878 |
6.860 |
-0.404 |
| z |
0.135 |
-0.404 |
4.348 |
<r2> (average value of r
2) Å
2
| <r2> |
186.769 |
| (<r2>)1/2 |
13.666 |