Jump to
S1C2
Energy calculated at G3B3
| | hartrees |
| Energy at 0K | -5225.666493 |
| Energy at 298.15K | -5225.660174 |
| HF Energy | -5226.392950 |
| Nuclear repulsion energy | 412.979010 |
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 B3LYP/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 |
3135 |
3011 |
0.00 |
|
|
|
| 2 |
Ag |
1518 |
1457 |
0.00 |
|
|
|
| 3 |
Ag |
1298 |
1246 |
0.00 |
|
|
|
| 4 |
Ag |
1071 |
1029 |
0.00 |
|
|
|
| 5 |
Ag |
654 |
628 |
0.00 |
|
|
|
| 6 |
Ag |
187 |
179 |
0.00 |
|
|
|
| 7 |
Au |
3219 |
3091 |
1.39 |
|
|
|
| 8 |
Au |
1105 |
1062 |
2.97 |
|
|
|
| 9 |
Au |
763 |
732 |
4.36 |
|
|
|
| 10 |
Au |
102 |
98 |
4.46 |
|
|
|
| 11 |
Bg |
3198 |
3071 |
0.00 |
|
|
|
| 12 |
Bg |
1302 |
1250 |
0.00 |
|
|
|
| 13 |
Bg |
941 |
904 |
0.00 |
|
|
|
| 14 |
Bu |
3143 |
3018 |
6.63 |
|
|
|
| 15 |
Bu |
1511 |
1451 |
5.80 |
|
|
|
| 16 |
Bu |
1221 |
1173 |
64.85 |
|
|
|
| 17 |
Bu |
580 |
557 |
80.11 |
|
|
|
| 18 |
Bu |
180 |
173 |
7.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12563.6 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 12064.8 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 B3LYP/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.497 |
0.569 |
0.000 |
| C2 |
-0.497 |
-0.569 |
0.000 |
| Br3 |
-0.497 |
2.285 |
0.000 |
| Br4 |
0.497 |
-2.285 |
0.000 |
| H5 |
1.119 |
0.576 |
0.894 |
| H6 |
1.119 |
0.576 |
-0.894 |
| H7 |
-1.119 |
-0.576 |
0.894 |
| H8 |
-1.119 |
-0.576 |
-0.894 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5103 | 1.9829 | 2.8535 | 1.0888 | 1.0888 | 2.1725 | 2.1725 |
C2 | 1.5103 | | 2.8535 | 1.9829 | 2.1725 | 2.1725 | 1.0888 | 1.0888 | Br3 | 1.9829 | 2.8535 | | 4.6762 | 2.5155 | 2.5155 | 3.0611 | 3.0611 | Br4 | 2.8535 | 1.9829 | 4.6762 | | 3.0611 | 3.0611 | 2.5155 | 2.5155 | H5 | 1.0888 | 2.1725 | 2.5155 | 3.0611 | | 1.7871 | 2.5170 | 3.0869 | H6 | 1.0888 | 2.1725 | 2.5155 | 3.0611 | 1.7871 | | 3.0869 | 2.5170 | H7 | 2.1725 | 1.0888 | 3.0611 | 2.5155 | 2.5170 | 3.0869 | | 1.7871 | H8 | 2.1725 | 1.0888 | 3.0611 | 2.5155 | 3.0869 | 2.5170 | 1.7871 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.300 |
|
C1 |
C2 |
H7 |
112.114 |
| C1 |
C2 |
H8 |
112.114 |
|
C2 |
C1 |
Br3 |
109.300 |
| C2 |
C1 |
H5 |
112.114 |
|
C2 |
C1 |
H6 |
112.114 |
| Br3 |
C1 |
H5 |
106.482 |
|
Br3 |
C1 |
H6 |
106.482 |
| Br4 |
C2 |
H7 |
106.482 |
|
Br4 |
C2 |
H8 |
106.482 |
| H5 |
C1 |
H6 |
110.032 |
|
H7 |
C2 |
H8 |
110.032 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.287 |
|
|
|
| 2 |
C |
-0.287 |
|
|
|
| 3 |
Br |
-0.132 |
|
|
|
| 4 |
Br |
-0.132 |
|
|
|
| 5 |
H |
0.210 |
|
|
|
| 6 |
H |
0.210 |
|
|
|
| 7 |
H |
0.210 |
|
|
|
| 8 |
H |
0.210 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
430.776 |
| (<r2>)1/2 |
20.755 |
Jump to
S1C1
Energy calculated at G3B3
| | hartrees |
| Energy at 0K | -5225.663775 |
| Energy at 298.15K | -5225.657633 |
| HF Energy | -5226.388566 |
| Nuclear repulsion energy | 444.820929 |
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 B3LYP/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 |
3176 |
3050 |
0.05 |
97.06 |
0.75 |
0.86 |
| 2 |
A |
3112 |
2989 |
16.21 |
205.62 |
0.02 |
0.04 |
| 3 |
A |
1498 |
1438 |
0.10 |
6.14 |
0.68 |
0.81 |
| 4 |
A |
1324 |
1271 |
27.24 |
4.47 |
0.58 |
0.74 |
| 5 |
A |
1198 |
1151 |
2.79 |
17.61 |
0.75 |
0.86 |
| 6 |
A |
1034 |
993 |
0.75 |
3.63 |
0.68 |
0.81 |
| 7 |
A |
913 |
877 |
7.39 |
7.54 |
0.47 |
0.64 |
| 8 |
A |
548 |
527 |
10.71 |
18.79 |
0.08 |
0.15 |
| 9 |
A |
226 |
217 |
1.15 |
1.12 |
0.27 |
0.43 |
| 10 |
A |
84 |
81 |
0.19 |
0.89 |
0.72 |
0.83 |
| 11 |
B |
3190 |
3063 |
2.30 |
27.88 |
0.75 |
0.86 |
| 12 |
B |
3104 |
2981 |
1.80 |
60.51 |
0.75 |
0.86 |
| 13 |
B |
1488 |
1429 |
8.86 |
18.11 |
0.75 |
0.86 |
| 14 |
B |
1291 |
1240 |
70.31 |
0.91 |
0.75 |
0.86 |
| 15 |
B |
1128 |
1083 |
2.13 |
5.78 |
0.75 |
0.86 |
| 16 |
B |
847 |
814 |
17.70 |
0.80 |
0.75 |
0.86 |
| 17 |
B |
582 |
559 |
14.69 |
10.14 |
0.75 |
0.86 |
| 18 |
B |
355 |
341 |
7.96 |
2.90 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12548.3 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 12050.2 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 B3LYP/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.307 |
0.690 |
1.218 |
| C2 |
-0.307 |
-0.690 |
1.218 |
| Br3 |
-0.307 |
1.784 |
-0.302 |
| Br4 |
0.307 |
-1.784 |
-0.302 |
| H5 |
0.006 |
1.235 |
2.115 |
| H6 |
1.394 |
0.657 |
1.149 |
| H7 |
-0.006 |
-1.235 |
2.115 |
| H8 |
-1.394 |
-0.657 |
1.149 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5116 | 1.9703 | 2.9034 | 1.0924 | 1.0893 | 2.1478 | 2.1712 |
C2 | 1.5116 | | 2.9034 | 1.9703 | 2.1478 | 2.1712 | 1.0924 | 1.0893 | Br3 | 1.9703 | 2.9034 | | 3.6196 | 2.4986 | 2.5041 | 3.8791 | 3.0399 | Br4 | 2.9034 | 1.9703 | 3.6196 | | 3.8791 | 3.0399 | 2.4986 | 2.5041 | H5 | 1.0924 | 2.1478 | 2.4986 | 3.8791 | | 1.7872 | 2.4707 | 2.5445 | H6 | 1.0893 | 2.1712 | 2.5041 | 3.0399 | 1.7872 | | 2.5445 | 3.0818 | H7 | 2.1478 | 1.0924 | 3.8791 | 2.4986 | 2.4707 | 2.5445 | | 1.7872 | H8 | 2.1712 | 1.0893 | 3.0399 | 2.5041 | 2.5445 | 3.0818 | 1.7872 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.478 |
|
C1 |
C2 |
H7 |
109.408 |
| C1 |
C2 |
H8 |
112.293 |
|
C2 |
C1 |
Br3 |
113.478 |
| C2 |
C1 |
H5 |
109.408 |
|
C2 |
C1 |
H6 |
112.293 |
| Br3 |
C1 |
H5 |
105.378 |
|
Br3 |
C1 |
H6 |
106.358 |
| Br4 |
C2 |
H7 |
105.378 |
|
Br4 |
C2 |
H8 |
106.358 |
| H5 |
C1 |
H6 |
109.642 |
|
H7 |
C2 |
H8 |
109.642 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.291 |
|
|
|
| 2 |
C |
-0.291 |
|
|
|
| 3 |
Br |
-0.116 |
|
|
|
| 4 |
Br |
-0.116 |
|
|
|
| 5 |
H |
0.198 |
|
|
|
| 6 |
H |
0.210 |
|
|
|
| 7 |
H |
0.198 |
|
|
|
| 8 |
H |
0.210 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.681 |
2.681 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
310.088 |
| (<r2>)1/2 |
17.609 |