Jump to
S1C2
Energy calculated at wB97X-D/3-21G*
| | hartrees |
| Energy at 0K | -5202.310149 |
| Energy at 298.15K | |
| HF Energy | -5202.310149 |
| Nuclear repulsion energy | 417.790382 |
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 wB97X-D/3-21G*
| 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 |
3152 |
2987 |
0.00 |
129.81 |
0.08 |
0.15 |
| 2 |
Ag |
1542 |
1462 |
0.00 |
22.27 |
0.75 |
0.86 |
| 3 |
Ag |
1341 |
1271 |
0.00 |
23.44 |
0.44 |
0.61 |
| 4 |
Ag |
1049 |
994 |
0.00 |
10.98 |
0.72 |
0.83 |
| 5 |
Ag |
722 |
685 |
0.00 |
66.06 |
0.29 |
0.45 |
| 6 |
Ag |
199 |
189 |
0.00 |
3.80 |
0.32 |
0.49 |
| 7 |
Au |
3238 |
3069 |
0.09 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1161 |
1101 |
3.45 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
787 |
746 |
8.61 |
0.00 |
0.26 |
0.41 |
| 10 |
Au |
106 |
101 |
3.98 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3215 |
3047 |
0.00 |
89.12 |
0.75 |
0.86 |
| 12 |
Bg |
1341 |
1271 |
0.00 |
11.21 |
0.75 |
0.86 |
| 13 |
Bg |
968 |
917 |
0.00 |
9.00 |
0.75 |
0.86 |
| 14 |
Bu |
3160 |
2995 |
4.00 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1541 |
1460 |
16.97 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1272 |
1206 |
36.23 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
654 |
620 |
53.77 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
188 |
178 |
6.16 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12818.0 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 12148.9 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 wB97X-D/3-21G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.498 |
0.575 |
0.000 |
| C2 |
-0.498 |
-0.575 |
0.000 |
| Br3 |
-0.498 |
2.258 |
0.000 |
| Br4 |
0.498 |
-2.258 |
0.000 |
| H5 |
1.118 |
0.565 |
0.895 |
| H6 |
1.118 |
0.565 |
-0.895 |
| H7 |
-1.118 |
-0.565 |
0.895 |
| H8 |
-1.118 |
-0.565 |
-0.895 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5213 | 1.9552 | 2.8326 | 1.0887 | 1.0887 | 2.1709 | 2.1709 |
C2 | 1.5213 | | 2.8326 | 1.9552 | 2.1709 | 2.1709 | 1.0887 | 1.0887 | Br3 | 1.9552 | 2.8326 | | 4.6237 | 2.5051 | 2.5051 | 3.0257 | 3.0257 | Br4 | 2.8326 | 1.9552 | 4.6237 | | 3.0257 | 3.0257 | 2.5051 | 2.5051 | H5 | 1.0887 | 2.1709 | 2.5051 | 3.0257 | | 1.7895 | 2.5059 | 3.0793 | H6 | 1.0887 | 2.1709 | 2.5051 | 3.0257 | 1.7895 | | 3.0793 | 2.5059 | H7 | 2.1709 | 1.0887 | 3.0257 | 2.5051 | 2.5059 | 3.0793 | | 1.7895 | H8 | 2.1709 | 1.0887 | 3.0257 | 2.5051 | 3.0793 | 2.5059 | 1.7895 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.488 |
|
C1 |
C2 |
H7 |
111.487 |
| C1 |
C2 |
H8 |
111.487 |
|
C2 |
C1 |
Br3 |
108.488 |
| C2 |
C1 |
H5 |
111.487 |
|
C2 |
C1 |
H6 |
111.487 |
| Br3 |
C1 |
H5 |
107.317 |
|
Br3 |
C1 |
H6 |
107.317 |
| Br4 |
C2 |
H7 |
107.317 |
|
Br4 |
C2 |
H8 |
107.317 |
| H5 |
C1 |
H6 |
110.543 |
|
H7 |
C2 |
H8 |
110.543 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.482 |
|
|
|
| 2 |
C |
-0.482 |
|
|
|
| 3 |
Br |
-0.069 |
|
|
|
| 4 |
Br |
-0.069 |
|
|
|
| 5 |
H |
0.276 |
|
|
|
| 6 |
H |
0.276 |
|
|
|
| 7 |
H |
0.276 |
|
|
|
| 8 |
H |
0.276 |
|
|
|
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 |
-47.763 |
0.895 |
0.000 |
| y |
0.895 |
-54.179 |
0.000 |
| z |
0.000 |
0.000 |
-48.661 |
|
| Traceless |
| | x | y | z |
| x |
3.657 |
0.895 |
0.000 |
| y |
0.895 |
-5.966 |
0.000 |
| z |
0.000 |
0.000 |
2.309 |
|
| Polar |
| 3z2-r2 | 4.618 |
| x2-y2 | 6.416 |
| xy | 0.895 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.164 |
-1.913 |
0.000 |
| y |
-1.913 |
10.989 |
0.000 |
| z |
0.000 |
0.000 |
5.225 |
<r2> (average value of r
2) Å
2
| <r2> |
421.905 |
| (<r2>)1/2 |
20.540 |
Jump to
S1C1
Energy calculated at wB97X-D/3-21G*
| | hartrees |
| Energy at 0K | -5202.307323 |
| Energy at 298.15K | |
| HF Energy | -5202.307323 |
| Nuclear repulsion energy | 457.880156 |
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 wB97X-D/3-21G*
| 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 |
3199 |
3032 |
0.02 |
95.51 |
0.74 |
0.85 |
| 2 |
A |
3139 |
2975 |
10.29 |
176.03 |
0.02 |
0.04 |
| 3 |
A |
1527 |
1447 |
1.02 |
8.10 |
0.71 |
0.83 |
| 4 |
A |
1359 |
1288 |
16.74 |
4.62 |
0.68 |
0.81 |
| 5 |
A |
1235 |
1171 |
1.42 |
19.01 |
0.75 |
0.86 |
| 6 |
A |
1031 |
978 |
1.51 |
2.93 |
0.75 |
0.86 |
| 7 |
A |
940 |
891 |
9.96 |
7.53 |
0.51 |
0.68 |
| 8 |
A |
602 |
571 |
6.46 |
17.34 |
0.09 |
0.17 |
| 9 |
A |
228 |
217 |
0.98 |
0.89 |
0.35 |
0.52 |
| 10 |
A |
81 |
77 |
0.17 |
0.87 |
0.73 |
0.84 |
| 11 |
B |
3214 |
3046 |
0.45 |
30.49 |
0.75 |
0.86 |
| 12 |
B |
3131 |
2968 |
1.46 |
48.53 |
0.75 |
0.86 |
| 13 |
B |
1530 |
1450 |
21.23 |
21.38 |
0.75 |
0.86 |
| 14 |
B |
1345 |
1275 |
33.98 |
0.57 |
0.75 |
0.86 |
| 15 |
B |
1182 |
1121 |
2.49 |
7.03 |
0.75 |
0.86 |
| 16 |
B |
872 |
826 |
21.12 |
1.05 |
0.75 |
0.86 |
| 17 |
B |
638 |
605 |
7.77 |
9.99 |
0.75 |
0.86 |
| 18 |
B |
369 |
349 |
5.34 |
2.85 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12810.9 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 12142.2 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 wB97X-D/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.305 |
0.697 |
1.224 |
| C2 |
-0.305 |
-0.697 |
1.224 |
| Br3 |
-0.305 |
1.741 |
-0.304 |
| Br4 |
0.305 |
-1.741 |
-0.304 |
| H5 |
-0.007 |
1.239 |
2.118 |
| H6 |
1.392 |
0.654 |
1.170 |
| H7 |
0.007 |
-1.239 |
2.118 |
| H8 |
-1.392 |
-0.654 |
1.170 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5215 | 1.9474 | 2.8766 | 1.0916 | 1.0893 | 2.1540 | 2.1690 |
C2 | 1.5215 | | 2.8766 | 1.9474 | 2.1540 | 2.1690 | 1.0916 | 1.0893 | Br3 | 1.9474 | 2.8766 | | 3.5339 | 2.4912 | 2.4959 | 3.8528 | 3.0141 | Br4 | 2.8766 | 1.9474 | 3.5339 | | 3.8528 | 3.0141 | 2.4912 | 2.4959 | H5 | 1.0916 | 2.1540 | 2.4912 | 3.8528 | | 1.7886 | 2.4790 | 2.5301 | H6 | 1.0893 | 2.1690 | 2.4959 | 3.0141 | 1.7886 | | 2.5301 | 3.0751 | H7 | 2.1540 | 1.0916 | 3.8528 | 2.4912 | 2.4790 | 2.5301 | | 1.7886 | H8 | 2.1690 | 1.0893 | 3.0141 | 2.4959 | 2.5301 | 3.0751 | 1.7886 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
111.456 |
|
C1 |
C2 |
H7 |
109.941 |
| C1 |
C2 |
H8 |
111.278 |
|
C2 |
C1 |
Br3 |
111.456 |
| C2 |
C1 |
H5 |
109.941 |
|
C2 |
C1 |
H6 |
111.278 |
| Br3 |
C1 |
H5 |
106.706 |
|
Br3 |
C1 |
H6 |
107.139 |
| Br4 |
C2 |
H7 |
106.706 |
|
Br4 |
C2 |
H8 |
107.139 |
| H5 |
C1 |
H6 |
110.187 |
|
H7 |
C2 |
H8 |
110.187 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.486 |
|
|
|
| 2 |
C |
-0.486 |
|
|
|
| 3 |
Br |
-0.055 |
|
|
|
| 4 |
Br |
-0.055 |
|
|
|
| 5 |
H |
0.266 |
|
|
|
| 6 |
H |
0.275 |
|
|
|
| 7 |
H |
0.266 |
|
|
|
| 8 |
H |
0.275 |
|
|
|
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 |
2.539 |
2.539 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.337 |
0.700 |
0.000 |
| y |
0.700 |
-52.274 |
0.000 |
| z |
0.000 |
0.000 |
-43.822 |
|
| Traceless |
| | x | y | z |
| x |
-0.289 |
0.700 |
0.000 |
| y |
0.700 |
-6.194 |
0.000 |
| z |
0.000 |
0.000 |
6.483 |
|
| Polar |
| 3z2-r2 | 12.967 |
| x2-y2 | 3.937 |
| xy | 0.700 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.538 |
-0.751 |
0.000 |
| y |
-0.751 |
8.082 |
0.000 |
| z |
0.000 |
0.000 |
7.614 |
<r2> (average value of r
2) Å
2
| <r2> |
299.499 |
| (<r2>)1/2 |
17.306 |