Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-311G**
| | hartrees |
| Energy at 0K | -1072.690390 |
| 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 | -1072.687465 |
| Energy at 298.15K | |
| HF Energy | -1072.392539 |
| Nuclear repulsion energy | 265.456989 |
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 |
3139 |
3139 |
5.46 |
80.77 |
0.21 |
0.34 |
| 2 |
A |
2971 |
2971 |
59.81 |
148.23 |
0.32 |
0.48 |
| 3 |
A |
1821 |
1821 |
128.58 |
13.24 |
0.56 |
0.72 |
| 4 |
A |
1411 |
1411 |
15.53 |
4.13 |
0.46 |
0.63 |
| 5 |
A |
1283 |
1283 |
18.96 |
4.57 |
0.68 |
0.81 |
| 6 |
A |
1249 |
1249 |
10.97 |
8.12 |
0.75 |
0.86 |
| 7 |
A |
1039 |
1039 |
14.68 |
2.39 |
0.47 |
0.64 |
| 8 |
A |
942 |
942 |
11.52 |
5.43 |
0.64 |
0.78 |
| 9 |
A |
813 |
813 |
84.20 |
7.22 |
0.72 |
0.84 |
| 10 |
A |
648 |
648 |
38.38 |
9.11 |
0.10 |
0.18 |
| 11 |
A |
618 |
618 |
38.06 |
7.73 |
0.45 |
0.62 |
| 12 |
A |
347 |
347 |
1.80 |
3.25 |
0.25 |
0.40 |
| 13 |
A |
280 |
280 |
2.68 |
6.13 |
0.65 |
0.79 |
| 14 |
A |
223 |
223 |
2.51 |
1.79 |
0.71 |
0.83 |
| 15 |
A |
88 |
88 |
10.23 |
2.28 |
0.73 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 8435.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8435.7 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=FULLultrafine/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.098 |
-0.024 |
0.518 |
| C2 |
-0.715 |
-1.285 |
0.196 |
| H3 |
0.226 |
0.057 |
1.596 |
| Cl4 |
1.740 |
-0.258 |
-0.168 |
| Cl5 |
-0.680 |
1.452 |
-0.057 |
| O6 |
-1.795 |
-1.286 |
-0.320 |
| H7 |
-0.192 |
-2.209 |
0.505 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5342 | 1.0883 | 1.7956 | 1.7646 | 2.4247 | 2.2039 |
C2 | 1.5342 | | 2.1552 | 2.6864 | 2.7488 | 1.1973 | 1.1057 | H3 | 1.0883 | 2.1552 | | 2.3463 | 2.3445 | 3.0918 | 2.5493 | Cl4 | 1.7956 | 2.6864 | 2.3463 | | 2.9654 | 3.6855 | 2.8272 | Cl5 | 1.7646 | 2.7488 | 2.3445 | 2.9654 | | 2.9686 | 3.7357 | O6 | 2.4247 | 1.1973 | 3.0918 | 3.6855 | 2.9686 | | 2.0255 | H7 | 2.2039 | 1.1057 | 2.5493 | 2.8272 | 3.7357 | 2.0255 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
124.710 |
|
C1 |
C2 |
H7 |
112.177 |
| C2 |
C1 |
H3 |
109.352 |
|
C2 |
C1 |
Cl4 |
107.304 |
| C2 |
C1 |
Cl5 |
112.689 |
|
H3 |
C1 |
Cl4 |
106.293 |
| H3 |
C1 |
Cl5 |
108.180 |
|
Cl4 |
C1 |
Cl5 |
112.800 |
| O6 |
C2 |
H7 |
123.111 |
|
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 |
-0.341 |
|
|
|
| 2 |
C |
0.225 |
|
|
|
| 3 |
H |
0.223 |
|
|
|
| 4 |
Cl |
-0.014 |
|
|
|
| 5 |
Cl |
0.015 |
|
|
|
| 6 |
O |
-0.220 |
|
|
|
| 7 |
H |
0.113 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.084 |
-0.895 |
1.957 |
2.410 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.275 |
-1.965 |
-1.219 |
| y |
-1.965 |
-42.401 |
-1.526 |
| z |
-1.219 |
-1.526 |
-40.976 |
|
| Traceless |
| | x | y | z |
| x |
-6.586 |
-1.965 |
-1.219 |
| y |
-1.965 |
2.224 |
-1.526 |
| z |
-1.219 |
-1.526 |
4.362 |
|
| Polar |
| 3z2-r2 | 8.725 |
| x2-y2 | -5.874 |
| xy | -1.965 |
| xz | -1.219 |
| yz | -1.526 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.015 |
-0.870 |
0.127 |
| y |
-0.870 |
6.896 |
-0.406 |
| z |
0.127 |
-0.406 |
4.369 |
<r2> (average value of r
2) Å
2
| <r2> |
186.759 |
| (<r2>)1/2 |
13.666 |