Jump to
S1C2
Energy calculated at CCD/6-311G**
| | hartrees |
| Energy at 0K | -5223.416482 |
| Energy at 298.15K | -5223.426754 |
| HF Energy | -5222.827779 |
| Nuclear repulsion energy | 417.160361 |
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 CCD/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 |
Ag |
3139 |
2998 |
0.00 |
|
|
|
| 2 |
Ag |
1513 |
1445 |
0.00 |
|
|
|
| 3 |
Ag |
1353 |
1292 |
0.00 |
|
|
|
| 4 |
Ag |
1091 |
1042 |
0.00 |
|
|
|
| 5 |
Ag |
719 |
686 |
0.00 |
|
|
|
| 6 |
Ag |
198 |
189 |
0.00 |
|
|
|
| 7 |
Au |
3220 |
3075 |
2.80 |
|
|
|
| 8 |
Au |
1150 |
1098 |
5.07 |
|
|
|
| 9 |
Au |
774 |
740 |
3.55 |
|
|
|
| 10 |
Au |
112 |
107 |
3.85 |
|
|
|
| 11 |
Bg |
3199 |
3055 |
0.00 |
|
|
|
| 12 |
Bg |
1322 |
1263 |
0.00 |
|
|
|
| 13 |
Bg |
983 |
939 |
0.00 |
|
|
|
| 14 |
Bu |
3145 |
3004 |
10.63 |
|
|
|
| 15 |
Bu |
1507 |
1439 |
4.97 |
|
|
|
| 16 |
Bu |
1261 |
1205 |
67.32 |
|
|
|
| 17 |
Bu |
639 |
610 |
45.53 |
|
|
|
| 18 |
Bu |
189 |
180 |
5.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12756.1 cm
-1
Scaled (by 0.9551) Zero Point Vibrational Energy (zpe) 12183.3 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 CCD/6-311G**
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.490 |
0.579 |
0.000 |
| C2 |
-0.490 |
-0.579 |
0.000 |
| Br3 |
-0.490 |
2.267 |
0.000 |
| Br4 |
0.490 |
-2.267 |
0.000 |
| H5 |
1.117 |
0.571 |
0.891 |
| H6 |
1.117 |
0.571 |
-0.891 |
| H7 |
-1.117 |
-0.571 |
0.891 |
| H8 |
-1.117 |
-0.571 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5176 | 1.9518 | 2.8458 | 1.0895 | 1.0895 | 2.1680 | 2.1680 |
C2 | 1.5176 | | 2.8458 | 1.9518 | 2.1680 | 2.1680 | 1.0895 | 1.0895 | Br3 | 1.9518 | 2.8458 | | 4.6382 | 2.5005 | 2.5005 | 3.0397 | 3.0397 | Br4 | 2.8458 | 1.9518 | 4.6382 | | 3.0397 | 3.0397 | 2.5005 | 2.5005 | H5 | 1.0895 | 2.1680 | 2.5005 | 3.0397 | | 1.7826 | 2.5087 | 3.0775 | H6 | 1.0895 | 2.1680 | 2.5005 | 3.0397 | 1.7826 | | 3.0775 | 2.5087 | H7 | 2.1680 | 1.0895 | 3.0397 | 2.5005 | 2.5087 | 3.0775 | | 1.7826 | H8 | 2.1680 | 1.0895 | 3.0397 | 2.5005 | 3.0775 | 2.5087 | 1.7826 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.590 |
|
C1 |
C2 |
H7 |
111.465 |
| C1 |
C2 |
H8 |
111.465 |
|
C2 |
C1 |
Br3 |
109.590 |
| C2 |
C1 |
H5 |
111.465 |
|
C2 |
C1 |
H6 |
111.465 |
| Br3 |
C1 |
H5 |
107.175 |
|
Br3 |
C1 |
H6 |
107.175 |
| Br4 |
C2 |
H7 |
107.175 |
|
Br4 |
C2 |
H8 |
107.175 |
| H5 |
C1 |
H6 |
109.787 |
|
H7 |
C2 |
H8 |
109.787 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at CCD/6-311G**
| | hartrees |
| Energy at 0K | -5223.413078 |
| Energy at 298.15K | |
| HF Energy | -5222.823599 |
| Nuclear repulsion energy | 450.918232 |
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 CCD/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 |
3183 |
3040 |
0.61 |
|
|
|
| 2 |
A |
3125 |
2984 |
19.67 |
|
|
|
| 3 |
A |
1498 |
1430 |
0.15 |
|
|
|
| 4 |
A |
1360 |
1299 |
24.30 |
|
|
|
| 5 |
A |
1232 |
1176 |
2.35 |
|
|
|
| 6 |
A |
1068 |
1020 |
0.07 |
|
|
|
| 7 |
A |
943 |
900 |
5.80 |
|
|
|
| 8 |
A |
586 |
560 |
6.11 |
|
|
|
| 9 |
A |
237 |
226 |
0.80 |
|
|
|
| 10 |
A |
85 |
81 |
0.21 |
|
|
|
| 11 |
B |
3195 |
3051 |
3.65 |
|
|
|
| 12 |
B |
3116 |
2976 |
3.16 |
|
|
|
| 13 |
B |
1489 |
1422 |
8.14 |
|
|
|
| 14 |
B |
1335 |
1275 |
66.21 |
|
|
|
| 15 |
B |
1159 |
1107 |
3.86 |
|
|
|
| 16 |
B |
876 |
836 |
13.96 |
|
|
|
| 17 |
B |
625 |
597 |
9.84 |
|
|
|
| 18 |
B |
368 |
351 |
4.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12738.2 cm
-1
Scaled (by 0.9551) Zero Point Vibrational Energy (zpe) 12166.3 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 CCD/6-311G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.310 |
0.693 |
1.177 |
| C2 |
-0.310 |
-0.693 |
1.177 |
| Br3 |
-0.310 |
1.806 |
-0.293 |
| Br4 |
0.310 |
-1.806 |
-0.293 |
| H5 |
0.027 |
1.212 |
2.095 |
| H6 |
1.397 |
0.644 |
1.106 |
| H7 |
-0.027 |
-1.212 |
2.095 |
| H8 |
-1.397 |
-0.644 |
1.106 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5190 | 1.9448 | 2.8993 | 1.0925 | 1.0901 | 2.1421 | 2.1694 |
C2 | 1.5190 | | 2.8993 | 1.9448 | 2.1421 | 2.1694 | 1.0925 | 1.0901 | Br3 | 1.9448 | 2.8993 | | 3.6646 | 2.4841 | 2.4942 | 3.8592 | 3.0231 | Br4 | 2.8993 | 1.9448 | 3.6646 | | 3.8592 | 3.0231 | 2.4841 | 2.4942 | H5 | 1.0925 | 2.1421 | 2.4841 | 3.8592 | | 1.7828 | 2.4249 | 2.5397 | H6 | 1.0901 | 2.1694 | 2.4942 | 3.0231 | 1.7828 | | 2.5397 | 3.0760 | H7 | 2.1421 | 1.0925 | 3.8592 | 2.4841 | 2.4249 | 2.5397 | | 1.7828 | H8 | 2.1694 | 1.0901 | 3.0231 | 2.4942 | 2.5397 | 3.0760 | 1.7828 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.082 |
|
C1 |
C2 |
H7 |
109.131 |
| C1 |
C2 |
H8 |
111.438 |
|
C2 |
C1 |
Br3 |
113.082 |
| C2 |
C1 |
H5 |
109.131 |
|
C2 |
C1 |
H6 |
111.438 |
| Br3 |
C1 |
H5 |
106.334 |
|
Br3 |
C1 |
H6 |
107.151 |
| Br4 |
C2 |
H7 |
106.334 |
|
Br4 |
C2 |
H8 |
107.151 |
| H5 |
C1 |
H6 |
109.536 |
|
H7 |
C2 |
H8 |
109.536 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability