Jump to
S1C2
Energy calculated at CCSD/6-311G*
| | hartrees |
| Energy at 0K | -3110.541960 |
| Energy at 298.15K | |
| HF Energy | -3109.958460 |
| Nuclear repulsion energy | 288.307894 |
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 CCSD/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' |
202 |
192 |
6.73 |
|
|
|
| 2 |
A' |
256 |
244 |
0.71 |
|
|
|
| 3 |
A' |
673 |
641 |
45.38 |
|
|
|
| 4 |
A' |
786 |
749 |
24.38 |
|
|
|
| 5 |
A' |
1094 |
1043 |
1.10 |
|
|
|
| 6 |
A' |
1281 |
1222 |
47.61 |
|
|
|
| 7 |
A' |
1386 |
1321 |
2.58 |
|
|
|
| 8 |
A' |
1518 |
1448 |
6.19 |
|
|
|
| 9 |
A' |
1520 |
1449 |
1.16 |
|
|
|
| 10 |
A' |
3117 |
2972 |
2.58 |
|
|
|
| 11 |
A' |
3125 |
2980 |
12.97 |
|
|
|
| 12 |
A" |
119 |
114 |
5.61 |
|
|
|
| 13 |
A" |
783 |
746 |
4.09 |
|
|
|
| 14 |
A" |
1018 |
971 |
0.25 |
|
|
|
| 15 |
A" |
1182 |
1127 |
4.55 |
|
|
|
| 16 |
A" |
1333 |
1271 |
0.20 |
|
|
|
| 17 |
A" |
3175 |
3028 |
0.55 |
|
|
|
| 18 |
A" |
3198 |
3049 |
4.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12881.6 cm
-1
Scaled (by 0.9535) Zero Point Vibrational Energy (zpe) 12282.6 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 CCSD/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.641 |
0.000 |
| C2 |
1.241 |
-0.231 |
0.000 |
| Br3 |
-1.593 |
-0.491 |
0.000 |
| Cl4 |
2.697 |
0.819 |
0.000 |
| H5 |
-0.049 |
1.267 |
0.892 |
| H6 |
-0.049 |
1.267 |
-0.892 |
| H7 |
1.286 |
-0.858 |
0.891 |
| H8 |
1.286 |
-0.858 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5170 | 1.9546 | 2.7027 | 1.0904 | 1.0904 | 2.1668 | 2.1668 |
C2 | 1.5170 | | 2.8467 | 1.7946 | 2.1688 | 2.1688 | 1.0908 | 1.0908 | Br3 | 1.9546 | 2.8467 | | 4.4858 | 2.5039 | 2.5039 | 3.0363 | 3.0363 | Cl4 | 2.7027 | 1.7946 | 4.4858 | | 2.9217 | 2.9217 | 2.3660 | 2.3660 | H5 | 1.0904 | 2.1688 | 2.5039 | 2.9217 | | 1.7833 | 2.5095 | 3.0784 | H6 | 1.0904 | 2.1688 | 2.5039 | 2.9217 | 1.7833 | | 3.0784 | 2.5095 | H7 | 2.1668 | 1.0908 | 3.0363 | 2.3660 | 2.5095 | 3.0784 | | 1.7826 | H8 | 2.1668 | 1.0908 | 3.0363 | 2.3660 | 3.0784 | 2.5095 | 1.7826 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.111 |
|
C1 |
C2 |
H7 |
111.335 |
| C1 |
C2 |
H8 |
111.335 |
|
C2 |
C1 |
Br3 |
109.524 |
| C2 |
C1 |
Cl4 |
38.859 |
|
C2 |
C1 |
H6 |
111.517 |
| Br3 |
C1 |
H5 |
107.192 |
|
Br3 |
C1 |
H6 |
107.192 |
| Cl4 |
C2 |
H7 |
107.660 |
|
Cl4 |
C2 |
H8 |
107.660 |
| H5 |
C1 |
H6 |
109.712 |
|
H7 |
C2 |
H8 |
109.599 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at CCSD/6-311G*
| | hartrees |
| Energy at 0K | -3110.539038 |
| Energy at 298.15K | |
| HF Energy | -3109.954873 |
| Nuclear repulsion energy | 304.190555 |
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 CCSD/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 |
3176 |
3028 |
4.35 |
|
|
|
| 2 |
A |
3159 |
3013 |
2.47 |
|
|
|
| 3 |
A |
3107 |
2963 |
18.23 |
|
|
|
| 4 |
A |
3093 |
2949 |
9.83 |
|
|
|
| 5 |
A |
1506 |
1436 |
1.18 |
|
|
|
| 6 |
A |
1500 |
1430 |
11.29 |
|
|
|
| 7 |
A |
1392 |
1327 |
25.70 |
|
|
|
| 8 |
A |
1349 |
1286 |
43.27 |
|
|
|
| 9 |
A |
1256 |
1197 |
3.88 |
|
|
|
| 10 |
A |
1187 |
1132 |
3.30 |
|
|
|
| 11 |
A |
1078 |
1028 |
0.94 |
|
|
|
| 12 |
A |
969 |
924 |
8.75 |
|
|
|
| 13 |
A |
904 |
862 |
20.60 |
|
|
|
| 14 |
A |
708 |
675 |
17.33 |
|
|
|
| 15 |
A |
595 |
568 |
9.65 |
|
|
|
| 16 |
A |
397 |
379 |
5.97 |
|
|
|
| 17 |
A |
251 |
239 |
1.02 |
|
|
|
| 18 |
A |
105 |
101 |
0.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12866.1 cm
-1
Scaled (by 0.9535) Zero Point Vibrational Energy (zpe) 12267.9 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 CCSD/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
1.098 |
-0.386 |
| C2 |
1.288 |
0.896 |
0.406 |
| Br3 |
-1.359 |
-0.224 |
0.036 |
| Cl4 |
2.174 |
-0.576 |
-0.087 |
| H5 |
-0.417 |
2.074 |
-0.144 |
| H6 |
0.195 |
1.036 |
-1.460 |
| H7 |
1.954 |
1.746 |
0.226 |
| H8 |
1.084 |
0.818 |
1.475 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5165 | 1.9503 | 2.7517 | 1.0928 | 1.0909 | 2.1373 | 2.1665 |
C2 | 1.5165 | | 2.8983 | 1.7876 | 2.1446 | 2.1670 | 1.0940 | 1.0914 | Br3 | 1.9503 | 2.8983 | | 3.5528 | 2.4903 | 2.4978 | 3.8588 | 3.0205 | Cl4 | 2.7517 | 1.7876 | 3.5528 | | 3.7070 | 2.8982 | 2.3532 | 2.3607 | H5 | 1.0928 | 2.1446 | 2.4903 | 3.7070 | | 1.7840 | 2.4220 | 2.5405 | H6 | 1.0909 | 2.1670 | 2.4978 | 2.8982 | 1.7840 | | 2.5376 | 3.0742 | H7 | 2.1373 | 1.0940 | 3.8588 | 2.3532 | 2.4220 | 2.5376 | | 1.7826 | H8 | 2.1665 | 1.0914 | 3.0205 | 2.3607 | 2.5405 | 3.0742 | 1.7826 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.521 |
|
C1 |
C2 |
H7 |
108.844 |
| C1 |
C2 |
H8 |
111.309 |
|
C2 |
C1 |
Br3 |
112.846 |
| C2 |
C1 |
Cl4 |
36.876 |
|
C2 |
C1 |
H6 |
111.373 |
| Br3 |
C1 |
H5 |
106.402 |
|
Br3 |
C1 |
H6 |
107.019 |
| Cl4 |
C2 |
H7 |
107.027 |
|
Cl4 |
C2 |
H8 |
107.702 |
| H5 |
C1 |
H6 |
109.557 |
|
H7 |
C2 |
H8 |
109.312 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability