Jump to
S1C2
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -5226.940357 |
| Energy at 298.15K | -5226.950630 |
| HF Energy | -5226.940357 |
| Nuclear repulsion energy | 418.176855 |
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 M06-2X/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 |
3158 |
3158 |
0.00 |
|
|
|
| 2 |
Ag |
1512 |
1512 |
0.00 |
|
|
|
| 3 |
Ag |
1335 |
1335 |
0.00 |
|
|
|
| 4 |
Ag |
1092 |
1092 |
0.00 |
|
|
|
| 5 |
Ag |
700 |
700 |
0.00 |
|
|
|
| 6 |
Ag |
197 |
197 |
0.00 |
|
|
|
| 7 |
Au |
3243 |
3243 |
0.22 |
|
|
|
| 8 |
Au |
1150 |
1150 |
6.08 |
|
|
|
| 9 |
Au |
778 |
778 |
5.81 |
|
|
|
| 10 |
Au |
125 |
125 |
4.77 |
|
|
|
| 11 |
Bg |
3222 |
3222 |
0.00 |
|
|
|
| 12 |
Bg |
1320 |
1320 |
0.00 |
|
|
|
| 13 |
Bg |
984 |
984 |
0.00 |
|
|
|
| 14 |
Bu |
3167 |
3167 |
5.74 |
|
|
|
| 15 |
Bu |
1506 |
1506 |
8.98 |
|
|
|
| 16 |
Bu |
1259 |
1259 |
64.90 |
|
|
|
| 17 |
Bu |
623 |
623 |
75.01 |
|
|
|
| 18 |
Bu |
195 |
195 |
7.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12782.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12782.0 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 M06-2X/6-311G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.494 |
0.570 |
0.000 |
| C2 |
-0.494 |
-0.570 |
0.000 |
| Br3 |
-0.494 |
2.257 |
0.000 |
| Br4 |
0.494 |
-2.257 |
0.000 |
| H5 |
1.116 |
0.570 |
0.891 |
| H6 |
1.116 |
0.570 |
-0.891 |
| H7 |
-1.116 |
-0.570 |
0.891 |
| H8 |
-1.116 |
-0.570 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5084 | 1.9559 | 2.8272 | 1.0864 | 1.0864 | 2.1648 | 2.1648 |
C2 | 1.5084 | | 2.8272 | 1.9559 | 2.1648 | 2.1648 | 1.0864 | 1.0864 | Br3 | 1.9559 | 2.8272 | | 4.6219 | 2.4965 | 2.4965 | 3.0294 | 3.0294 | Br4 | 2.8272 | 1.9559 | 4.6219 | | 3.0294 | 3.0294 | 2.4965 | 2.4965 | H5 | 1.0864 | 2.1648 | 2.4965 | 3.0294 | | 1.7816 | 2.5068 | 3.0754 | H6 | 1.0864 | 2.1648 | 2.4965 | 3.0294 | 1.7816 | | 3.0754 | 2.5068 | H7 | 2.1648 | 1.0864 | 3.0294 | 2.4965 | 2.5068 | 3.0754 | | 1.7816 | H8 | 2.1648 | 1.0864 | 3.0294 | 2.4965 | 3.0754 | 2.5068 | 1.7816 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.699 |
|
C1 |
C2 |
H7 |
112.063 |
| C1 |
C2 |
H8 |
112.063 |
|
C2 |
C1 |
Br3 |
108.699 |
| C2 |
C1 |
H5 |
112.063 |
|
C2 |
C1 |
H6 |
112.063 |
| Br3 |
C1 |
H5 |
106.778 |
|
Br3 |
C1 |
H6 |
106.778 |
| Br4 |
C2 |
H7 |
106.778 |
|
Br4 |
C2 |
H8 |
106.778 |
| H5 |
C1 |
H6 |
110.167 |
|
H7 |
C2 |
H8 |
110.167 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.546 |
|
|
|
| 2 |
C |
-0.546 |
|
|
|
| 3 |
Br |
-0.039 |
|
|
|
| 4 |
Br |
-0.039 |
|
|
|
| 5 |
H |
0.293 |
|
|
|
| 6 |
H |
0.293 |
|
|
|
| 7 |
H |
0.293 |
|
|
|
| 8 |
H |
0.293 |
|
|
|
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
| Primitive |
| | x | y | z |
| x |
-49.233 |
1.357 |
0.000 |
| y |
1.357 |
-56.585 |
0.000 |
| z |
0.000 |
0.000 |
-49.885 |
|
| Traceless |
| | x | y | z |
| x |
4.002 |
1.357 |
0.000 |
| y |
1.357 |
-7.026 |
0.000 |
| z |
0.000 |
0.000 |
3.024 |
|
| Polar |
| 3z2-r2 | 6.047 |
| x2-y2 | 7.352 |
| xy | 1.357 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.620 |
-2.112 |
0.000 |
| y |
-2.112 |
12.430 |
0.000 |
| z |
0.000 |
0.000 |
5.353 |
<r2> (average value of r
2) Å
2
| <r2> |
422.531 |
| (<r2>)1/2 |
20.556 |
Jump to
S1C1
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -5226.937321 |
| Energy at 298.15K | |
| HF Energy | -5226.937321 |
| Nuclear repulsion energy | 453.094018 |
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 M06-2X/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 |
3190 |
3190 |
0.01 |
96.26 |
0.75 |
0.86 |
| 2 |
A |
3130 |
3130 |
14.12 |
208.17 |
0.02 |
0.04 |
| 3 |
A |
1490 |
1490 |
0.87 |
4.50 |
0.59 |
0.74 |
| 4 |
A |
1341 |
1341 |
25.71 |
3.73 |
0.64 |
0.78 |
| 5 |
A |
1226 |
1226 |
2.63 |
14.07 |
0.75 |
0.86 |
| 6 |
A |
1057 |
1057 |
0.20 |
2.72 |
0.70 |
0.82 |
| 7 |
A |
932 |
932 |
9.59 |
7.90 |
0.45 |
0.62 |
| 8 |
A |
580 |
580 |
9.75 |
18.22 |
0.08 |
0.15 |
| 9 |
A |
238 |
238 |
1.03 |
1.58 |
0.52 |
0.68 |
| 10 |
A |
84 |
84 |
0.23 |
1.40 |
0.72 |
0.84 |
| 11 |
B |
3202 |
3202 |
1.00 |
28.59 |
0.75 |
0.86 |
| 12 |
B |
3124 |
3124 |
2.45 |
47.05 |
0.75 |
0.86 |
| 13 |
B |
1483 |
1483 |
13.85 |
13.53 |
0.75 |
0.86 |
| 14 |
B |
1311 |
1311 |
66.60 |
1.40 |
0.75 |
0.86 |
| 15 |
B |
1154 |
1154 |
4.24 |
5.66 |
0.75 |
0.86 |
| 16 |
B |
869 |
869 |
23.15 |
1.51 |
0.75 |
0.86 |
| 17 |
B |
616 |
616 |
16.24 |
11.20 |
0.75 |
0.86 |
| 18 |
B |
367 |
367 |
6.50 |
2.69 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12696.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12696.8 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 M06-2X/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.308 |
0.689 |
1.188 |
| C2 |
-0.308 |
-0.689 |
1.188 |
| Br3 |
-0.308 |
1.788 |
-0.295 |
| Br4 |
0.308 |
-1.788 |
-0.295 |
| H5 |
0.019 |
1.218 |
2.095 |
| H6 |
1.392 |
0.648 |
1.118 |
| H7 |
-0.019 |
-1.218 |
2.095 |
| H8 |
-1.392 |
-0.648 |
1.118 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5097 | 1.9463 | 2.8876 | 1.0892 | 1.0870 | 2.1372 | 2.1638 |
C2 | 1.5097 | | 2.8876 | 1.9463 | 2.1372 | 2.1638 | 1.0892 | 1.0870 | Br3 | 1.9463 | 2.8876 | | 3.6293 | 2.4791 | 2.4879 | 3.8519 | 3.0180 | Br4 | 2.8876 | 1.9463 | 3.6293 | | 3.8519 | 3.0180 | 2.4791 | 2.4879 | H5 | 1.0892 | 2.1372 | 2.4791 | 3.8519 | | 1.7790 | 2.4368 | 2.5350 | H6 | 1.0870 | 2.1638 | 2.4879 | 3.0180 | 1.7790 | | 2.5350 | 3.0706 | H7 | 2.1372 | 1.0892 | 3.8519 | 2.4791 | 2.4368 | 2.5350 | | 1.7790 | H8 | 2.1638 | 1.0870 | 3.0180 | 2.4879 | 2.5350 | 3.0706 | 1.7790 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
112.733 |
|
C1 |
C2 |
H7 |
109.580 |
| C1 |
C2 |
H8 |
111.852 |
|
C2 |
C1 |
Br3 |
112.733 |
| C2 |
C1 |
H5 |
109.580 |
|
C2 |
C1 |
H6 |
111.852 |
| Br3 |
C1 |
H5 |
106.038 |
|
Br3 |
C1 |
H6 |
106.760 |
| Br4 |
C2 |
H7 |
106.038 |
|
Br4 |
C2 |
H8 |
106.760 |
| H5 |
C1 |
H6 |
109.671 |
|
H7 |
C2 |
H8 |
109.671 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.548 |
|
|
|
| 2 |
C |
-0.548 |
|
|
|
| 3 |
Br |
-0.025 |
|
|
|
| 4 |
Br |
-0.025 |
|
|
|
| 5 |
H |
0.282 |
|
|
|
| 6 |
H |
0.291 |
|
|
|
| 7 |
H |
0.282 |
|
|
|
| 8 |
H |
0.291 |
|
|
|
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 |
2.783 |
2.783 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.661 |
0.904 |
0.000 |
| y |
0.904 |
-54.368 |
0.000 |
| z |
0.000 |
0.000 |
-45.246 |
|
| Traceless |
| | x | y | z |
| x |
0.146 |
0.904 |
0.000 |
| y |
0.904 |
-6.915 |
0.000 |
| z |
0.000 |
0.000 |
6.769 |
|
| Polar |
| 3z2-r2 | 13.537 |
| x2-y2 | 4.707 |
| xy | 0.904 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.855 |
-0.813 |
0.000 |
| y |
-0.813 |
9.090 |
0.000 |
| z |
0.000 |
0.000 |
8.133 |
<r2> (average value of r
2) Å
2
| <r2> |
310.433 |
| (<r2>)1/2 |
17.619 |