Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -1073.125046 |
| Energy at 298.15K | -1073.127556 |
| HF Energy | -1073.125046 |
| Nuclear repulsion energy | 264.414417 |
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 B1B95/6-311G*
| 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' |
3196 |
3064 |
1.78 |
|
|
|
| 2 |
A' |
2991 |
2867 |
51.27 |
|
|
|
| 3 |
A' |
1875 |
1797 |
184.67 |
|
|
|
| 4 |
A' |
1416 |
1358 |
4.70 |
|
|
|
| 5 |
A' |
1233 |
1182 |
11.19 |
|
|
|
| 6 |
A' |
1074 |
1030 |
30.81 |
|
|
|
| 7 |
A' |
798 |
765 |
24.34 |
|
|
|
| 8 |
A' |
443 |
425 |
5.29 |
|
|
|
| 9 |
A' |
321 |
308 |
23.53 |
|
|
|
| 10 |
A' |
259 |
248 |
2.78 |
|
|
|
| 11 |
A" |
1278 |
1225 |
23.04 |
|
|
|
| 12 |
A" |
1026 |
983 |
22.03 |
|
|
|
| 13 |
A" |
740 |
709 |
140.16 |
|
|
|
| 14 |
A" |
275 |
264 |
3.65 |
|
|
|
| 15 |
A" |
89 |
86 |
7.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8507.0 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 8154.8 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 B1B95/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.386 |
-0.020 |
0.000 |
| C2 |
-0.170 |
1.394 |
0.000 |
| H3 |
1.470 |
-0.002 |
0.000 |
| Cl4 |
-0.170 |
-0.839 |
1.470 |
| Cl5 |
-0.170 |
-0.839 |
-1.470 |
| O6 |
0.537 |
2.353 |
0.000 |
| H7 |
-1.273 |
1.450 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5193 | 1.0838 | 1.7723 | 1.7723 | 2.3778 | 2.2166 |
C2 | 1.5193 | | 2.1540 | 2.6731 | 2.6731 | 1.1917 | 1.1045 | H3 | 1.0838 | 2.1540 | | 2.3560 | 2.3560 | 2.5336 | 3.1038 | Cl4 | 1.7723 | 2.6731 | 2.3560 | | 2.9399 | 3.5846 | 2.9350 | Cl5 | 1.7723 | 2.6731 | 2.3560 | 2.9399 | | 3.5846 | 2.9350 | O6 | 2.3778 | 1.1917 | 2.5336 | 3.5846 | 3.5846 | | 2.0232 | H7 | 2.2166 | 1.1045 | 3.1038 | 2.9350 | 2.9350 | 2.0232 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
122.121 |
|
C1 |
C2 |
H7 |
114.373 |
| C2 |
C1 |
H3 |
110.561 |
|
C2 |
C1 |
Cl4 |
108.359 |
| C2 |
C1 |
Cl5 |
108.359 |
|
H3 |
C1 |
Cl4 |
108.747 |
| H3 |
C1 |
Cl5 |
108.747 |
|
Cl4 |
C1 |
Cl5 |
112.074 |
| O6 |
C2 |
H7 |
123.506 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.516 |
|
|
|
| 2 |
C |
0.178 |
|
|
|
| 3 |
H |
0.336 |
|
|
|
| 4 |
Cl |
0.019 |
|
|
|
| 5 |
Cl |
0.019 |
|
|
|
| 6 |
O |
-0.247 |
|
|
|
| 7 |
H |
0.211 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.304 |
-0.544 |
0.000 |
0.623 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-41.012 |
-2.803 |
0.000 |
| y |
-2.803 |
-48.529 |
0.000 |
| z |
0.000 |
0.000 |
-43.133 |
|
| Traceless |
| | x | y | z |
| x |
4.820 |
-2.803 |
0.000 |
| y |
-2.803 |
-6.457 |
0.000 |
| z |
0.000 |
0.000 |
1.637 |
|
| Polar |
| 3z2-r2 | 3.275 |
| x2-y2 | 7.518 |
| xy | -2.803 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.053 |
0.704 |
0.000 |
| y |
0.704 |
6.994 |
0.000 |
| z |
0.000 |
0.000 |
7.503 |
<r2> (average value of r
2) Å
2
| <r2> |
191.212 |
| (<r2>)1/2 |
13.828 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -1073.122372 |
| Energy at 298.15K | |
| HF Energy | -1073.122372 |
| Nuclear repulsion energy | 267.167851 |
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 B1B95/6-311G*
| 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 |
3140 |
3010 |
6.19 |
81.72 |
0.21 |
0.35 |
| 2 |
A |
2975 |
2852 |
63.63 |
145.20 |
0.33 |
0.49 |
| 3 |
A |
1888 |
1810 |
157.57 |
15.45 |
0.52 |
0.69 |
| 4 |
A |
1410 |
1352 |
17.03 |
3.86 |
0.55 |
0.71 |
| 5 |
A |
1285 |
1232 |
18.09 |
4.56 |
0.70 |
0.82 |
| 6 |
A |
1248 |
1197 |
9.87 |
8.53 |
0.75 |
0.85 |
| 7 |
A |
1039 |
996 |
15.93 |
2.04 |
0.51 |
0.67 |
| 8 |
A |
944 |
904 |
10.61 |
5.73 |
0.62 |
0.76 |
| 9 |
A |
822 |
788 |
90.81 |
6.58 |
0.71 |
0.83 |
| 10 |
A |
655 |
628 |
40.80 |
8.31 |
0.10 |
0.18 |
| 11 |
A |
622 |
596 |
37.72 |
7.31 |
0.41 |
0.59 |
| 12 |
A |
344 |
330 |
1.88 |
2.87 |
0.27 |
0.42 |
| 13 |
A |
277 |
266 |
3.12 |
6.05 |
0.66 |
0.80 |
| 14 |
A |
217 |
208 |
2.64 |
1.72 |
0.70 |
0.83 |
| 15 |
A |
92 |
88 |
10.44 |
2.13 |
0.72 |
0.83 |
Unscaled Zero Point Vibrational Energy (zpe) 8479.4 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 8128.4 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 B1B95/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.099 |
-0.020 |
0.517 |
| C2 |
-0.699 |
-1.281 |
0.197 |
| H3 |
0.229 |
0.066 |
1.593 |
| Cl4 |
1.731 |
-0.245 |
-0.168 |
| Cl5 |
-0.689 |
1.437 |
-0.058 |
| O6 |
-1.770 |
-1.290 |
-0.318 |
| H7 |
-0.174 |
-2.205 |
0.502 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
Cl4 |
Cl5 |
O6 |
H7 |
| C1 | | 1.5267 | 1.0880 | 1.7840 | 1.7525 | 2.4089 | 2.2019 |
C2 | 1.5267 | | 2.1515 | 2.6669 | 2.7297 | 1.1884 | 1.1055 | H3 | 1.0880 | 2.1515 | | 2.3353 | 2.3337 | 3.0806 | 2.5516 | Cl4 | 1.7840 | 2.6669 | 2.3353 | | 2.9486 | 3.6569 | 2.8138 | Cl5 | 1.7525 | 2.7297 | 2.3337 | 2.9486 | | 2.9443 | 3.7198 | O6 | 2.4089 | 1.1884 | 3.0806 | 3.6569 | 2.9443 | | 2.0149 | H7 | 2.2019 | 1.1055 | 2.5516 | 2.8138 | 3.7198 | 2.0149 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O6 |
124.587 |
|
C1 |
C2 |
H7 |
112.565 |
| C2 |
C1 |
H3 |
109.601 |
|
C2 |
C1 |
Cl4 |
107.072 |
| C2 |
C1 |
Cl5 |
112.519 |
|
H3 |
C1 |
Cl4 |
106.264 |
| H3 |
C1 |
Cl5 |
108.201 |
|
Cl4 |
C1 |
Cl5 |
112.976 |
| O6 |
C2 |
H7 |
122.848 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.509 |
|
|
|
| 2 |
C |
0.157 |
|
|
|
| 3 |
H |
0.329 |
|
|
|
| 4 |
Cl |
0.007 |
|
|
|
| 5 |
Cl |
0.036 |
|
|
|
| 6 |
O |
-0.229 |
|
|
|
| 7 |
H |
0.209 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.136 |
-0.868 |
1.994 |
2.453 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.747 |
-2.048 |
-1.182 |
| y |
-2.048 |
-41.876 |
-1.548 |
| z |
-1.182 |
-1.548 |
-40.516 |
|
| Traceless |
| | x | y | z |
| x |
-6.550 |
-2.048 |
-1.182 |
| y |
-2.048 |
2.255 |
-1.548 |
| z |
-1.182 |
-1.548 |
4.295 |
|
| Polar |
| 3z2-r2 | 8.591 |
| x2-y2 | -5.870 |
| xy | -2.048 |
| xz | -1.182 |
| yz | -1.548 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.970 |
-0.846 |
0.136 |
| y |
-0.846 |
6.856 |
-0.392 |
| z |
0.136 |
-0.392 |
4.352 |
<r2> (average value of r
2) Å
2
| <r2> |
184.331 |
| (<r2>)1/2 |
13.577 |