Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -1072.805403 |
| 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/6-311+G(3df,2p)
Geometric Data calculated at B2PLYP=FULLultrafine/6-311+G(3df,2p)
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -1072.802212 |
| Energy at 298.15K | |
| HF Energy | -1072.421203 |
| Nuclear repulsion energy | 266.779531 |
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/6-311+G(3df,2p)
| 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 |
3116 |
3116 |
5.51 |
77.24 |
0.16 |
0.27 |
| 2 |
A |
2967 |
2967 |
45.81 |
130.37 |
0.28 |
0.44 |
| 3 |
A |
1812 |
1812 |
133.68 |
18.23 |
0.39 |
0.56 |
| 4 |
A |
1402 |
1402 |
11.76 |
3.22 |
0.33 |
0.50 |
| 5 |
A |
1274 |
1274 |
10.32 |
2.07 |
0.74 |
0.85 |
| 6 |
A |
1224 |
1224 |
10.83 |
4.34 |
0.68 |
0.81 |
| 7 |
A |
1034 |
1034 |
15.14 |
1.97 |
0.37 |
0.54 |
| 8 |
A |
942 |
942 |
8.56 |
3.08 |
0.57 |
0.72 |
| 9 |
A |
811 |
811 |
71.96 |
5.68 |
0.70 |
0.83 |
| 10 |
A |
651 |
651 |
33.54 |
12.92 |
0.07 |
0.13 |
| 11 |
A |
618 |
618 |
32.45 |
5.83 |
0.43 |
0.60 |
| 12 |
A |
344 |
344 |
1.74 |
3.34 |
0.12 |
0.21 |
| 13 |
A |
277 |
277 |
3.34 |
3.15 |
0.61 |
0.76 |
| 14 |
A |
219 |
219 |
2.92 |
1.00 |
0.63 |
0.77 |
| 15 |
A |
88 |
88 |
10.05 |
1.36 |
0.73 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 8389.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8389.5 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/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.096 |
-0.020 |
0.521 |
| C2 |
-0.713 |
-1.277 |
0.204 |
| H3 |
0.229 |
0.065 |
1.596 |
| Cl4 |
1.725 |
-0.263 |
-0.170 |
| Cl5 |
-0.669 |
1.449 |
-0.058 |
| O6 |
-1.785 |
-1.281 |
-0.325 |
| H7 |
-0.198 |
-2.200 |
0.521 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5279 | 1.0870 | 1.7858 | 1.7538 | 2.4175 | 2.2002 |
C2 | 1.5279 | | 2.1506 | 2.6660 | 2.7387 | 1.1960 | 1.1032 | H3 | 1.0870 | 2.1506 | | 2.3380 | 2.3356 | 3.0916 | 2.5438 | Cl4 | 1.7858 | 2.6660 | 2.3380 | | 2.9449 | 3.6578 | 2.8153 | Cl5 | 1.7538 | 2.7387 | 2.3356 | 2.9449 | | 2.9614 | 3.7244 | O6 | 2.4175 | 1.1960 | 3.0916 | 3.6578 | 2.9614 | | 2.0195 | H7 | 2.2002 | 1.1032 | 2.5438 | 2.8153 | 3.7244 | 2.0195 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
124.678 |
|
C1 |
C2 |
H7 |
112.488 |
| C2 |
C1 |
H3 |
109.504 |
|
C2 |
C1 |
Cl4 |
106.869 |
| C2 |
C1 |
Cl5 |
112.953 |
|
H3 |
C1 |
Cl4 |
106.383 |
| H3 |
C1 |
Cl5 |
108.303 |
|
Cl4 |
C1 |
Cl5 |
112.604 |
| O6 |
C2 |
H7 |
122.833 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.240 |
|
|
|
| 2 |
C |
0.716 |
|
|
|
| 3 |
H |
0.227 |
|
|
|
| 4 |
Cl |
-0.163 |
|
|
|
| 5 |
Cl |
-0.174 |
|
|
|
| 6 |
O |
-0.531 |
|
|
|
| 7 |
H |
0.165 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.320 |
-0.698 |
1.929 |
2.439 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.034 |
-2.176 |
-1.394 |
| y |
-2.176 |
-42.110 |
-1.672 |
| z |
-1.394 |
-1.672 |
-40.775 |
|
| Traceless |
| | x | y | z |
| x |
-6.592 |
-2.176 |
-1.394 |
| y |
-2.176 |
2.294 |
-1.672 |
| z |
-1.394 |
-1.672 |
4.297 |
|
| Polar |
| 3z2-r2 | 8.595 |
| x2-y2 | -5.924 |
| xy | -2.176 |
| xz | -1.394 |
| yz | -1.672 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.647 |
-0.527 |
0.216 |
| y |
-0.527 |
8.661 |
-0.220 |
| z |
0.216 |
-0.220 |
6.516 |
<r2> (average value of r
2) Å
2
| <r2> |
184.825 |
| (<r2>)1/2 |
13.595 |