Jump to
S1C2
Energy calculated at HSEh1PBE/6-31+G**
| | hartrees |
| Energy at 0K | -5221.272657 |
| Energy at 298.15K | |
| HF Energy | -5221.272657 |
| Nuclear repulsion energy | 418.681858 |
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/6-31+G**
| 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 |
2994 |
0.00 |
|
|
|
| 2 |
Ag |
1494 |
1426 |
0.00 |
|
|
|
| 3 |
Ag |
1309 |
1250 |
0.00 |
|
|
|
| 4 |
Ag |
1094 |
1044 |
0.00 |
|
|
|
| 5 |
Ag |
688 |
657 |
0.00 |
|
|
|
| 6 |
Ag |
195 |
186 |
0.00 |
|
|
|
| 7 |
Au |
3224 |
3079 |
0.01 |
|
|
|
| 8 |
Au |
1126 |
1076 |
4.13 |
|
|
|
| 9 |
Au |
768 |
733 |
4.39 |
|
|
|
| 10 |
Au |
132 |
126 |
4.66 |
|
|
|
| 11 |
Bg |
3202 |
3057 |
0.00 |
|
|
|
| 12 |
Bg |
1299 |
1240 |
0.00 |
|
|
|
| 13 |
Bg |
965 |
921 |
0.00 |
|
|
|
| 14 |
Bu |
3143 |
3001 |
4.78 |
|
|
|
| 15 |
Bu |
1487 |
1420 |
8.95 |
|
|
|
| 16 |
Bu |
1229 |
1174 |
57.74 |
|
|
|
| 17 |
Bu |
615 |
587 |
72.47 |
|
|
|
| 18 |
Bu |
176 |
168 |
7.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12639.3 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 12068.0 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/6-31+G**
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.489 |
0.571 |
0.000 |
| C2 |
-0.489 |
-0.571 |
0.000 |
| Br3 |
-0.489 |
2.257 |
0.000 |
| Br4 |
0.489 |
-2.257 |
0.000 |
| H5 |
1.115 |
0.575 |
0.892 |
| H6 |
1.115 |
0.575 |
-0.892 |
| H7 |
-1.115 |
-0.575 |
0.892 |
| H8 |
-1.115 |
-0.575 |
-0.892 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5044 | 1.9493 | 2.8280 | 1.0896 | 1.0896 | 2.1645 | 2.1645 |
C2 | 1.5044 | | 2.8280 | 1.9493 | 2.1645 | 2.1645 | 1.0896 | 1.0896 | Br3 | 1.9493 | 2.8280 | | 4.6186 | 2.4897 | 2.4897 | 3.0345 | 3.0345 | Br4 | 2.8280 | 1.9493 | 4.6186 | | 3.0345 | 3.0345 | 2.4897 | 2.4897 | H5 | 1.0896 | 2.1645 | 2.4897 | 3.0345 | | 1.7834 | 2.5102 | 3.0792 | H6 | 1.0896 | 2.1645 | 2.4897 | 3.0345 | 1.7834 | | 3.0792 | 2.5102 | H7 | 2.1645 | 1.0896 | 3.0345 | 2.4897 | 2.5102 | 3.0792 | | 1.7834 | H8 | 2.1645 | 1.0896 | 3.0345 | 2.4897 | 3.0792 | 2.5102 | 1.7834 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.264 |
|
C1 |
C2 |
H7 |
112.132 |
| C1 |
C2 |
H8 |
112.132 |
|
C2 |
C1 |
Br3 |
109.264 |
| C2 |
C1 |
H5 |
112.132 |
|
C2 |
C1 |
H6 |
112.132 |
| Br3 |
C1 |
H5 |
106.576 |
|
Br3 |
C1 |
H6 |
106.576 |
| Br4 |
C2 |
H7 |
106.576 |
|
Br4 |
C2 |
H8 |
106.576 |
| H5 |
C1 |
H6 |
109.855 |
|
H7 |
C2 |
H8 |
109.855 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.311 |
|
|
|
| 2 |
C |
-0.311 |
|
|
|
| 3 |
Br |
-0.128 |
|
|
|
| 4 |
Br |
-0.128 |
|
|
|
| 5 |
H |
0.219 |
|
|
|
| 6 |
H |
0.219 |
|
|
|
| 7 |
H |
0.219 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
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 |
-49.124 |
1.334 |
0.000 |
| y |
1.334 |
-56.204 |
0.000 |
| z |
0.000 |
0.000 |
-49.875 |
|
| Traceless |
| | x | y | z |
| x |
3.916 |
1.334 |
0.000 |
| y |
1.334 |
-6.704 |
0.000 |
| z |
0.000 |
0.000 |
2.789 |
|
| Polar |
| 3z2-r2 | 5.577 |
| x2-y2 | 7.080 |
| xy | 1.334 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.003 |
-1.743 |
0.000 |
| y |
-1.743 |
13.355 |
0.000 |
| z |
0.000 |
0.000 |
7.202 |
<r2> (average value of r
2) Å
2
| <r2> |
421.884 |
| (<r2>)1/2 |
20.540 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31+G**
| | hartrees |
| Energy at 0K | -5221.269844 |
| Energy at 298.15K | |
| HF Energy | -5221.269844 |
| Nuclear repulsion energy | 452.357680 |
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/6-31+G**
| 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 |
3185 |
3041 |
0.01 |
94.13 |
0.75 |
0.86 |
| 2 |
A |
3117 |
2976 |
13.00 |
231.01 |
0.02 |
0.04 |
| 3 |
A |
1477 |
1410 |
1.01 |
4.48 |
0.75 |
0.85 |
| 4 |
A |
1329 |
1269 |
23.38 |
6.21 |
0.39 |
0.56 |
| 5 |
A |
1214 |
1159 |
1.75 |
11.23 |
0.74 |
0.85 |
| 6 |
A |
1064 |
1016 |
0.23 |
2.76 |
0.62 |
0.77 |
| 7 |
A |
925 |
883 |
8.11 |
7.25 |
0.22 |
0.36 |
| 8 |
A |
572 |
547 |
8.49 |
19.96 |
0.06 |
0.12 |
| 9 |
A |
243 |
232 |
1.18 |
1.52 |
0.17 |
0.29 |
| 10 |
A |
72 |
69 |
0.23 |
0.66 |
0.72 |
0.84 |
| 11 |
B |
3197 |
3053 |
0.14 |
28.35 |
0.75 |
0.86 |
| 12 |
B |
3109 |
2969 |
2.01 |
46.51 |
0.75 |
0.86 |
| 13 |
B |
1470 |
1403 |
16.32 |
13.30 |
0.75 |
0.86 |
| 14 |
B |
1293 |
1234 |
68.54 |
1.27 |
0.75 |
0.86 |
| 15 |
B |
1141 |
1089 |
2.76 |
2.76 |
0.75 |
0.86 |
| 16 |
B |
866 |
827 |
20.18 |
1.01 |
0.75 |
0.86 |
| 17 |
B |
605 |
578 |
16.65 |
9.15 |
0.75 |
0.86 |
| 18 |
B |
372 |
355 |
6.45 |
2.08 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12625.3 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 12054.7 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/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.318 |
0.682 |
1.169 |
| C2 |
-0.318 |
-0.682 |
1.169 |
| Br3 |
-0.318 |
1.799 |
-0.291 |
| Br4 |
0.318 |
-1.799 |
-0.291 |
| H5 |
0.051 |
1.211 |
2.087 |
| H6 |
1.403 |
0.627 |
1.079 |
| H7 |
-0.051 |
-1.211 |
2.087 |
| H8 |
-1.403 |
-0.627 |
1.079 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5043 | 1.9454 | 2.8781 | 1.0927 | 1.0901 | 2.1354 | 2.1639 |
C2 | 1.5043 | | 2.8781 | 1.9454 | 2.1354 | 2.1639 | 1.0927 | 1.0901 | Br3 | 1.9454 | 2.8781 | | 3.6534 | 2.4769 | 2.4925 | 3.8449 | 2.9895 | Br4 | 2.8781 | 1.9454 | 3.6534 | | 3.8449 | 2.9895 | 2.4769 | 2.4925 | H5 | 1.0927 | 2.1354 | 2.4769 | 3.8449 | | 1.7848 | 2.4241 | 2.5509 | H6 | 1.0901 | 2.1639 | 2.4925 | 2.9895 | 1.7848 | | 2.5509 | 3.0735 | H7 | 2.1354 | 1.0927 | 3.8449 | 2.4769 | 2.4241 | 2.5509 | | 1.7848 | H8 | 2.1639 | 1.0901 | 2.9895 | 2.4925 | 2.5509 | 3.0735 | 1.7848 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
112.462 |
|
C1 |
C2 |
H7 |
109.607 |
| C1 |
C2 |
H8 |
112.056 |
|
C2 |
C1 |
Br3 |
112.462 |
| C2 |
C1 |
H5 |
109.607 |
|
C2 |
C1 |
H6 |
112.056 |
| Br3 |
C1 |
H5 |
105.784 |
|
Br3 |
C1 |
H6 |
106.996 |
| Br4 |
C2 |
H7 |
105.784 |
|
Br4 |
C2 |
H8 |
106.996 |
| H5 |
C1 |
H6 |
109.709 |
|
H7 |
C2 |
H8 |
109.709 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.302 |
|
|
|
| 2 |
C |
-0.302 |
|
|
|
| 3 |
Br |
-0.123 |
|
|
|
| 4 |
Br |
-0.123 |
|
|
|
| 5 |
H |
0.206 |
|
|
|
| 6 |
H |
0.219 |
|
|
|
| 7 |
H |
0.206 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
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 |
2.730 |
2.730 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.554 |
0.979 |
0.000 |
| y |
0.979 |
-54.452 |
0.000 |
| z |
0.000 |
0.000 |
-45.149 |
|
| Traceless |
| | x | y | z |
| x |
0.247 |
0.979 |
0.000 |
| y |
0.979 |
-7.101 |
0.000 |
| z |
0.000 |
0.000 |
6.854 |
|
| Polar |
| 3z2-r2 | 13.708 |
| x2-y2 | 4.898 |
| xy | 0.979 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.571 |
-0.750 |
0.000 |
| y |
-0.750 |
10.553 |
0.000 |
| z |
0.000 |
0.000 |
9.081 |
<r2> (average value of r
2) Å
2
| <r2> |
312.440 |
| (<r2>)1/2 |
17.676 |