Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G*
| | hartrees |
| Energy at 0K | -5221.233797 |
| Energy at 298.15K | -5221.243958 |
| HF Energy | -5221.233797 |
| Nuclear repulsion energy | 418.124017 |
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 HSEh1PBE/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 |
3150 |
2996 |
0.00 |
|
|
|
| 2 |
Ag |
1515 |
1440 |
0.00 |
|
|
|
| 3 |
Ag |
1305 |
1241 |
0.00 |
|
|
|
| 4 |
Ag |
1096 |
1042 |
0.00 |
|
|
|
| 5 |
Ag |
681 |
648 |
0.00 |
|
|
|
| 6 |
Ag |
193 |
183 |
0.00 |
|
|
|
| 7 |
Au |
3238 |
3080 |
0.48 |
|
|
|
| 8 |
Au |
1116 |
1061 |
3.40 |
|
|
|
| 9 |
Au |
762 |
725 |
5.00 |
|
|
|
| 10 |
Au |
106 |
101 |
4.44 |
|
|
|
| 11 |
Bg |
3216 |
3059 |
0.00 |
|
|
|
| 12 |
Bg |
1306 |
1242 |
0.00 |
|
|
|
| 13 |
Bg |
949 |
902 |
0.00 |
|
|
|
| 14 |
Bu |
3158 |
3003 |
5.80 |
|
|
|
| 15 |
Bu |
1506 |
1433 |
7.88 |
|
|
|
| 16 |
Bu |
1225 |
1165 |
55.14 |
|
|
|
| 17 |
Bu |
610 |
580 |
72.90 |
|
|
|
| 18 |
Bu |
182 |
173 |
7.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12657.1 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 12036.9 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 HSEh1PBE/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.493 |
0.569 |
0.000 |
| C2 |
-0.493 |
-0.569 |
0.000 |
| Br3 |
-0.493 |
2.258 |
0.000 |
| Br4 |
0.493 |
-2.258 |
0.000 |
| H5 |
1.118 |
0.571 |
0.893 |
| H6 |
1.118 |
0.571 |
-0.893 |
| H7 |
-1.118 |
-0.571 |
0.893 |
| H8 |
-1.118 |
-0.571 |
-0.893 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5053 | 1.9562 | 2.8265 | 1.0894 | 1.0894 | 2.1654 | 2.1654 |
C2 | 1.5053 | | 2.8265 | 1.9562 | 2.1654 | 2.1654 | 1.0894 | 1.0894 | Br3 | 1.9562 | 2.8265 | | 4.6224 | 2.4978 | 2.4978 | 3.0310 | 3.0310 | Br4 | 2.8265 | 1.9562 | 4.6224 | | 3.0310 | 3.0310 | 2.4978 | 2.4978 | H5 | 1.0894 | 2.1654 | 2.4978 | 3.0310 | | 1.7853 | 2.5097 | 3.0799 | H6 | 1.0894 | 2.1654 | 2.4978 | 3.0310 | 1.7853 | | 3.0799 | 2.5097 | H7 | 2.1654 | 1.0894 | 3.0310 | 2.4978 | 2.5097 | 3.0799 | | 1.7853 | H8 | 2.1654 | 1.0894 | 3.0310 | 2.4978 | 3.0799 | 2.5097 | 1.7853 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.783 |
|
C1 |
C2 |
H7 |
112.145 |
| C1 |
C2 |
H8 |
112.145 |
|
C2 |
C1 |
Br3 |
108.783 |
| C2 |
C1 |
H5 |
112.145 |
|
C2 |
C1 |
H6 |
112.145 |
| Br3 |
C1 |
H5 |
106.707 |
|
Br3 |
C1 |
H6 |
106.707 |
| Br4 |
C2 |
H7 |
106.707 |
|
Br4 |
C2 |
H8 |
106.707 |
| H5 |
C1 |
H6 |
110.050 |
|
H7 |
C2 |
H8 |
110.050 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.352 |
|
|
|
| 2 |
C |
-0.352 |
|
|
|
| 3 |
Br |
-0.121 |
|
|
|
| 4 |
Br |
-0.121 |
|
|
|
| 5 |
H |
0.236 |
|
|
|
| 6 |
H |
0.236 |
|
|
|
| 7 |
H |
0.236 |
|
|
|
| 8 |
H |
0.236 |
|
|
|
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 |
-48.127 |
1.208 |
0.000 |
| y |
1.208 |
-54.962 |
0.000 |
| z |
0.000 |
0.000 |
-48.885 |
|
| Traceless |
| | x | y | z |
| x |
3.797 |
1.208 |
0.000 |
| y |
1.208 |
-6.456 |
0.000 |
| z |
0.000 |
0.000 |
2.659 |
|
| Polar |
| 3z2-r2 | 5.319 |
| x2-y2 | 6.835 |
| xy | 1.208 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.780 |
-1.808 |
0.000 |
| y |
-1.808 |
12.063 |
0.000 |
| z |
0.000 |
0.000 |
5.898 |
<r2> (average value of r
2) Å
2
| <r2> |
421.832 |
| (<r2>)1/2 |
20.539 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G*
| | hartrees |
| Energy at 0K | -5221.231344 |
| Energy at 298.15K | |
| HF Energy | -5221.231344 |
| Nuclear repulsion energy | 457.017525 |
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 HSEh1PBE/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 |
3197 |
3040 |
0.03 |
97.94 |
0.75 |
0.86 |
| 2 |
A |
3131 |
2977 |
14.56 |
204.29 |
0.02 |
0.04 |
| 3 |
A |
1495 |
1421 |
0.39 |
5.80 |
0.69 |
0.81 |
| 4 |
A |
1330 |
1265 |
24.80 |
4.25 |
0.63 |
0.77 |
| 5 |
A |
1211 |
1152 |
2.15 |
16.50 |
0.75 |
0.86 |
| 6 |
A |
1051 |
999 |
0.57 |
3.77 |
0.68 |
0.81 |
| 7 |
A |
923 |
878 |
7.41 |
6.65 |
0.46 |
0.63 |
| 8 |
A |
575 |
547 |
9.39 |
17.28 |
0.08 |
0.15 |
| 9 |
A |
230 |
218 |
1.07 |
0.94 |
0.30 |
0.46 |
| 10 |
A |
88 |
84 |
0.18 |
0.78 |
0.72 |
0.84 |
| 11 |
B |
3210 |
3053 |
1.24 |
30.81 |
0.75 |
0.86 |
| 12 |
B |
3123 |
2970 |
1.81 |
55.66 |
0.75 |
0.86 |
| 13 |
B |
1485 |
1412 |
11.95 |
17.39 |
0.75 |
0.86 |
| 14 |
B |
1295 |
1232 |
57.86 |
0.59 |
0.75 |
0.86 |
| 15 |
B |
1137 |
1081 |
2.31 |
5.62 |
0.75 |
0.86 |
| 16 |
B |
853 |
812 |
18.58 |
0.93 |
0.75 |
0.86 |
| 17 |
B |
606 |
577 |
12.17 |
8.99 |
0.75 |
0.86 |
| 18 |
B |
362 |
344 |
7.10 |
2.45 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12650.9 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 12031.0 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 HSEh1PBE/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.303 |
0.689 |
1.211 |
| C2 |
-0.303 |
-0.689 |
1.211 |
| Br3 |
-0.303 |
1.754 |
-0.301 |
| Br4 |
0.303 |
-1.754 |
-0.301 |
| H5 |
-0.002 |
1.233 |
2.109 |
| H6 |
1.391 |
0.655 |
1.151 |
| H7 |
0.002 |
-1.233 |
2.109 |
| H8 |
-1.391 |
-0.655 |
1.151 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5063 | 1.9457 | 2.8731 | 1.0927 | 1.0899 | 2.1430 | 2.1633 |
C2 | 1.5063 | | 2.8731 | 1.9457 | 2.1430 | 2.1633 | 1.0927 | 1.0899 | Br3 | 1.9457 | 2.8731 | | 3.5591 | 2.4836 | 2.4868 | 3.8495 | 3.0155 | Br4 | 2.8731 | 1.9457 | 3.5591 | | 3.8495 | 3.0155 | 2.4836 | 2.4868 | H5 | 1.0927 | 2.1430 | 2.4836 | 3.8495 | | 1.7860 | 2.4661 | 2.5320 | H6 | 1.0899 | 2.1633 | 2.4868 | 3.0155 | 1.7860 | | 2.5320 | 3.0745 | H7 | 2.1430 | 1.0927 | 3.8495 | 2.4836 | 2.4661 | 2.5320 | | 1.7860 | H8 | 2.1633 | 1.0899 | 3.0155 | 2.4868 | 2.5320 | 3.0745 | 1.7860 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
112.048 |
|
C1 |
C2 |
H7 |
110.076 |
| C1 |
C2 |
H8 |
111.871 |
|
C2 |
C1 |
Br3 |
112.048 |
| C2 |
C1 |
H5 |
110.076 |
|
C2 |
C1 |
H6 |
111.871 |
| Br3 |
C1 |
H5 |
106.229 |
|
Br3 |
C1 |
H6 |
106.584 |
| Br4 |
C2 |
H7 |
106.229 |
|
Br4 |
C2 |
H8 |
106.584 |
| H5 |
C1 |
H6 |
109.824 |
|
H7 |
C2 |
H8 |
109.824 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.355 |
|
|
|
| 2 |
C |
-0.355 |
|
|
|
| 3 |
Br |
-0.106 |
|
|
|
| 4 |
Br |
-0.106 |
|
|
|
| 5 |
H |
0.225 |
|
|
|
| 6 |
H |
0.236 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.236 |
|
|
|
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 |
2.672 |
2.672 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.607 |
0.853 |
0.000 |
| y |
0.853 |
-52.923 |
0.000 |
| z |
0.000 |
0.000 |
-44.087 |
|
| Traceless |
| | x | y | z |
| x |
-0.102 |
0.853 |
0.000 |
| y |
0.853 |
-6.576 |
0.000 |
| z |
0.000 |
0.000 |
6.678 |
|
| Polar |
| 3z2-r2 | 13.356 |
| x2-y2 | 4.316 |
| xy | 0.853 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.181 |
-0.718 |
0.000 |
| y |
-0.718 |
9.056 |
0.000 |
| z |
0.000 |
0.000 |
8.134 |
<r2> (average value of r
2) Å
2
| <r2> |
302.055 |
| (<r2>)1/2 |
17.380 |