Jump to
S1C2
Energy calculated at G3
| | hartrees |
| Energy at 0K | -998.649343 |
| Energy at 298.15K | -998.643437 |
| Nuclear repulsion energy | 194.751520 |
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 HF/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3303 |
3112 |
0.00 |
|
|
|
| 2 |
Ag |
1641 |
1546 |
0.00 |
|
|
|
| 3 |
Ag |
1496 |
1409 |
0.00 |
|
|
|
| 4 |
Ag |
1139 |
1073 |
0.00 |
|
|
|
| 5 |
Ag |
838 |
790 |
0.00 |
|
|
|
| 6 |
Ag |
324 |
305 |
0.00 |
|
|
|
| 7 |
Au |
3384 |
3188 |
7.35 |
|
|
|
| 8 |
Au |
1269 |
1195 |
1.12 |
|
|
|
| 9 |
Au |
840 |
791 |
1.70 |
|
|
|
| 10 |
Au |
128 |
120 |
9.27 |
|
|
|
| 11 |
Bg |
3362 |
3168 |
0.00 |
|
|
|
| 12 |
Bg |
1424 |
1341 |
0.00 |
|
|
|
| 13 |
Bg |
1117 |
1053 |
0.00 |
|
|
|
| 14 |
Bu |
3309 |
3118 |
23.78 |
|
|
|
| 15 |
Bu |
1638 |
1544 |
7.98 |
|
|
|
| 16 |
Bu |
1400 |
1319 |
58.90 |
|
|
|
| 17 |
Bu |
781 |
736 |
140.32 |
|
|
|
| 18 |
Bu |
236 |
223 |
11.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13813.8 cm
-1
Scaled (by 0.9422) Zero Point Vibrational Energy (zpe) 13015.4 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 MP2=FULL/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.757 |
0.000 |
| C2 |
0.000 |
-0.757 |
0.000 |
| Cl3 |
-1.682 |
1.348 |
0.000 |
| Cl4 |
1.682 |
-1.348 |
0.000 |
| H5 |
0.495 |
1.147 |
0.889 |
| H6 |
0.495 |
1.147 |
-0.889 |
| H7 |
-0.495 |
-1.147 |
0.889 |
| H8 |
-0.495 |
-1.147 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5133 | 1.7828 | 2.6939 | 1.0897 | 1.0897 | 2.1584 | 2.1584 |
C2 | 1.5133 | | 2.6939 | 1.7828 | 2.1584 | 2.1584 | 1.0897 | 1.0897 | Cl3 | 1.7828 | 2.6939 | | 4.3105 | 2.3604 | 2.3604 | 2.9017 | 2.9017 | Cl4 | 2.6939 | 1.7828 | 4.3105 | | 2.9017 | 2.9017 | 2.3604 | 2.3604 | H5 | 1.0897 | 2.1584 | 2.3604 | 2.9017 | | 1.7774 | 2.4987 | 3.0663 | H6 | 1.0897 | 2.1584 | 2.3604 | 2.9017 | 1.7774 | | 3.0663 | 2.4987 | H7 | 2.1584 | 1.0897 | 2.9017 | 2.3604 | 2.4987 | 3.0663 | | 1.7774 | H8 | 2.1584 | 1.0897 | 2.9017 | 2.3604 | 3.0663 | 2.4987 | 1.7774 | |
More geometry information
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at G3
| | hartrees |
| Energy at 0K | -998.647474 |
| Energy at 298.15K | -998.652706 |
| HF Energy | -997.027890 |
| Nuclear repulsion energy | 201.846377 |
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 HF/6-31G*
| 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 |
3347 |
3154 |
1.22 |
|
|
|
| 2 |
A |
3290 |
3100 |
32.35 |
|
|
|
| 3 |
A |
1627 |
1533 |
0.01 |
|
|
|
| 4 |
A |
1493 |
1407 |
32.40 |
|
|
|
| 5 |
A |
1360 |
1282 |
0.82 |
|
|
|
| 6 |
A |
1138 |
1072 |
0.50 |
|
|
|
| 7 |
A |
1043 |
982 |
15.82 |
|
|
|
| 8 |
A |
716 |
674 |
31.47 |
|
|
|
| 9 |
A |
281 |
264 |
0.88 |
|
|
|
| 10 |
A |
122 |
115 |
1.43 |
|
|
|
| 11 |
B |
3359 |
3165 |
8.12 |
|
|
|
| 12 |
B |
3279 |
3089 |
4.70 |
|
|
|
| 13 |
B |
1621 |
1527 |
9.12 |
|
|
|
| 14 |
B |
1467 |
1382 |
58.44 |
|
|
|
| 15 |
B |
1285 |
1211 |
0.88 |
|
|
|
| 16 |
B |
988 |
931 |
19.53 |
|
|
|
| 17 |
B |
747 |
704 |
42.25 |
|
|
|
| 18 |
B |
443 |
417 |
9.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13802.5 cm
-1
Scaled (by 0.9422) Zero Point Vibrational Energy (zpe) 13004.7 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 MP2=FULL/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.293 |
0.697 |
0.891 |
| C2 |
-0.293 |
-0.697 |
0.891 |
| Cl3 |
-0.293 |
1.681 |
-0.470 |
| Cl4 |
0.293 |
-1.681 |
-0.470 |
| H5 |
-0.002 |
1.205 |
1.812 |
| H6 |
1.381 |
0.661 |
0.834 |
| H7 |
0.002 |
-1.205 |
1.812 |
| H8 |
-1.381 |
-0.661 |
0.834 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5119 | 1.7784 | 2.7394 | 1.0921 | 1.0902 | 2.1328 | 2.1560 |
C2 | 1.5119 | | 2.7394 | 1.7784 | 2.1328 | 2.1560 | 1.0921 | 1.0902 | Cl3 | 1.7784 | 2.7394 | | 3.4118 | 2.3491 | 2.3542 | 3.6903 | 2.8927 | Cl4 | 2.7394 | 1.7784 | 3.4118 | | 3.6903 | 2.8927 | 2.3491 | 2.3542 | H5 | 1.0921 | 2.1328 | 2.3491 | 3.6903 | | 1.7784 | 2.4092 | 2.5177 | H6 | 1.0902 | 2.1560 | 2.3542 | 2.8927 | 1.7784 | | 2.5177 | 3.0619 | H7 | 2.1328 | 1.0921 | 3.6903 | 2.3491 | 2.4092 | 2.5177 | | 1.7784 | H8 | 2.1560 | 1.0902 | 2.8927 | 2.3542 | 2.5177 | 3.0619 | 1.7784 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.923 |
|
C1 |
C2 |
H7 |
108.961 |
| C1 |
C2 |
H8 |
111.367 |
|
C2 |
C1 |
Cl3 |
112.923 |
| C2 |
C1 |
H5 |
108.961 |
|
C2 |
C1 |
H6 |
111.367 |
| Cl3 |
C1 |
H5 |
106.722 |
|
Cl3 |
C1 |
H6 |
107.415 |
| Cl4 |
C2 |
H7 |
106.722 |
|
Cl4 |
C2 |
H8 |
107.415 |
| H5 |
C1 |
H6 |
109.300 |
|
H7 |
C2 |
H8 |
109.300 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability