Jump to
S1C2
Energy calculated at HSEh1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -5226.333761 |
| Energy at 298.15K | |
| HF Energy | -5226.333761 |
| Nuclear repulsion energy | 418.741220 |
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/aug-cc-pVTZ
| 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 |
3119 |
3000 |
0.00 |
163.49 |
0.02 |
0.04 |
| 2 |
Ag |
1482 |
1426 |
0.00 |
5.55 |
0.74 |
0.85 |
| 3 |
Ag |
1279 |
1230 |
0.00 |
49.31 |
0.29 |
0.45 |
| 4 |
Ag |
1086 |
1044 |
0.00 |
7.93 |
0.73 |
0.85 |
| 5 |
Ag |
680 |
654 |
0.00 |
100.93 |
0.25 |
0.40 |
| 6 |
Ag |
192 |
184 |
0.00 |
4.40 |
0.20 |
0.34 |
| 7 |
Au |
3203 |
3081 |
0.04 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1102 |
1060 |
2.40 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
757 |
728 |
3.75 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
102 |
98 |
4.33 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3179 |
3058 |
0.00 |
69.97 |
0.75 |
0.86 |
| 12 |
Bg |
1286 |
1237 |
0.00 |
1.76 |
0.75 |
0.86 |
| 13 |
Bg |
946 |
910 |
0.00 |
0.80 |
0.75 |
0.86 |
| 14 |
Bu |
3127 |
3008 |
4.22 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1477 |
1421 |
8.53 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1205 |
1159 |
46.29 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
612 |
589 |
70.35 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
178 |
172 |
6.77 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12506.3 cm
-1
Scaled (by 0.9618) Zero Point Vibrational Energy (zpe) 12028.5 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/aug-cc-pVTZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.491 |
0.567 |
0.000 |
| C2 |
-0.491 |
-0.567 |
0.000 |
| Br3 |
-0.491 |
2.256 |
0.000 |
| Br4 |
0.491 |
-2.256 |
0.000 |
| H5 |
1.113 |
0.573 |
0.890 |
| H6 |
1.113 |
0.573 |
-0.890 |
| H7 |
-1.113 |
-0.573 |
0.890 |
| H8 |
-1.113 |
-0.573 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4998 | 1.9536 | 2.8229 | 1.0858 | 1.0858 | 2.1597 | 2.1597 |
C2 | 1.4998 | | 2.8229 | 1.9536 | 2.1597 | 2.1597 | 1.0858 | 1.0858 | Br3 | 1.9536 | 2.8229 | | 4.6175 | 2.4890 | 2.4890 | 3.0305 | 3.0305 | Br4 | 2.8229 | 1.9536 | 4.6175 | | 3.0305 | 3.0305 | 2.4890 | 2.4890 | H5 | 1.0858 | 2.1597 | 2.4890 | 3.0305 | | 1.7796 | 2.5040 | 3.0720 | H6 | 1.0858 | 2.1597 | 2.4890 | 3.0305 | 1.7796 | | 3.0720 | 2.5040 | H7 | 2.1597 | 1.0858 | 3.0305 | 2.4890 | 2.5040 | 3.0720 | | 1.7796 | H8 | 2.1597 | 1.0858 | 3.0305 | 2.4890 | 3.0720 | 2.5040 | 1.7796 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.952 |
|
C1 |
C2 |
H7 |
112.304 |
| C1 |
C2 |
H8 |
112.304 |
|
C2 |
C1 |
Br3 |
108.952 |
| C2 |
C1 |
H5 |
112.304 |
|
C2 |
C1 |
H6 |
112.304 |
| Br3 |
C1 |
H5 |
106.429 |
|
Br3 |
C1 |
H6 |
106.429 |
| Br4 |
C2 |
H7 |
106.429 |
|
Br4 |
C2 |
H8 |
106.429 |
| H5 |
C1 |
H6 |
110.073 |
|
H7 |
C2 |
H8 |
110.073 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.362 |
|
|
|
| 2 |
C |
-0.362 |
|
|
|
| 3 |
Br |
-0.094 |
|
|
|
| 4 |
Br |
-0.094 |
|
|
|
| 5 |
H |
0.228 |
|
|
|
| 6 |
H |
0.228 |
|
|
|
| 7 |
H |
0.228 |
|
|
|
| 8 |
H |
0.228 |
|
|
|
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 |
-49.041 |
1.387 |
0.000 |
| y |
1.387 |
-55.913 |
0.000 |
| z |
0.000 |
0.000 |
-49.596 |
|
| Traceless |
| | x | y | z |
| x |
3.714 |
1.387 |
0.000 |
| y |
1.387 |
-6.594 |
0.000 |
| z |
0.000 |
0.000 |
2.880 |
|
| Polar |
| 3z2-r2 | 5.761 |
| x2-y2 | 6.872 |
| xy | 1.387 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.310 |
-1.612 |
0.000 |
| y |
-1.612 |
14.812 |
0.000 |
| z |
0.000 |
0.000 |
8.436 |
<r2> (average value of r
2) Å
2
| <r2> |
421.484 |
| (<r2>)1/2 |
20.530 |
Jump to
S1C1
Energy calculated at HSEh1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -5226.330329 |
| Energy at 298.15K | |
| HF Energy | -5226.330329 |
| Nuclear repulsion energy | 452.821356 |
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/aug-cc-pVTZ
| 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 |
3160 |
3039 |
0.01 |
81.76 |
0.75 |
0.86 |
| 2 |
A |
3101 |
2982 |
12.36 |
261.61 |
0.02 |
0.04 |
| 3 |
A |
1459 |
1403 |
1.15 |
2.80 |
0.74 |
0.85 |
| 4 |
A |
1307 |
1257 |
16.62 |
5.54 |
0.12 |
0.21 |
| 5 |
A |
1195 |
1149 |
0.86 |
5.29 |
0.75 |
0.86 |
| 6 |
A |
1048 |
1008 |
1.21 |
1.12 |
0.54 |
0.70 |
| 7 |
A |
911 |
876 |
6.98 |
4.42 |
0.18 |
0.30 |
| 8 |
A |
572 |
551 |
6.89 |
22.22 |
0.05 |
0.09 |
| 9 |
A |
228 |
219 |
1.24 |
1.36 |
0.19 |
0.32 |
| 10 |
A |
77 |
74 |
0.22 |
0.70 |
0.60 |
0.75 |
| 11 |
B |
3174 |
3053 |
0.23 |
26.84 |
0.75 |
0.86 |
| 12 |
B |
3092 |
2974 |
2.02 |
38.82 |
0.75 |
0.86 |
| 13 |
B |
1455 |
1399 |
14.02 |
8.40 |
0.75 |
0.86 |
| 14 |
B |
1275 |
1226 |
59.73 |
3.72 |
0.75 |
0.86 |
| 15 |
B |
1124 |
1081 |
1.22 |
1.06 |
0.75 |
0.86 |
| 16 |
B |
849 |
817 |
18.72 |
1.10 |
0.75 |
0.86 |
| 17 |
B |
605 |
582 |
14.30 |
7.31 |
0.75 |
0.86 |
| 18 |
B |
358 |
344 |
6.01 |
1.59 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12494.9 cm
-1
Scaled (by 0.9618) Zero Point Vibrational Energy (zpe) 12017.6 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/aug-cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.308 |
0.684 |
1.176 |
| C2 |
-0.308 |
-0.684 |
1.176 |
| Br3 |
-0.308 |
1.797 |
-0.293 |
| Br4 |
0.308 |
-1.797 |
-0.293 |
| H5 |
0.025 |
1.213 |
2.086 |
| H6 |
1.391 |
0.645 |
1.100 |
| H7 |
-0.025 |
-1.213 |
2.086 |
| H8 |
-1.391 |
-0.645 |
1.100 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5008 | 1.9432 | 2.8831 | 1.0892 | 1.0865 | 2.1300 | 2.1589 |
C2 | 1.5008 | | 2.8831 | 1.9432 | 2.1300 | 2.1589 | 1.0892 | 1.0865 | Br3 | 1.9432 | 2.8831 | | 3.6456 | 2.4716 | 2.4808 | 3.8462 | 3.0118 | Br4 | 2.8831 | 1.9432 | 3.6456 | | 3.8462 | 3.0118 | 2.4716 | 2.4808 | H5 | 1.0892 | 2.1300 | 2.4716 | 3.8462 | | 1.7780 | 2.4263 | 2.5358 | H6 | 1.0865 | 2.1589 | 2.4808 | 3.0118 | 1.7780 | | 2.5358 | 3.0670 | H7 | 2.1300 | 1.0892 | 3.8462 | 2.4716 | 2.4263 | 2.5358 | | 1.7780 | H8 | 2.1589 | 1.0865 | 3.0118 | 2.4808 | 2.5358 | 3.0670 | 1.7780 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.049 |
|
C1 |
C2 |
H7 |
109.623 |
| C1 |
C2 |
H8 |
112.114 |
|
C2 |
C1 |
Br3 |
113.049 |
| C2 |
C1 |
H5 |
109.623 |
|
C2 |
C1 |
H6 |
112.114 |
| Br3 |
C1 |
H5 |
105.714 |
|
Br3 |
C1 |
H6 |
106.483 |
| Br4 |
C2 |
H7 |
105.714 |
|
Br4 |
C2 |
H8 |
106.483 |
| H5 |
C1 |
H6 |
109.606 |
|
H7 |
C2 |
H8 |
109.606 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.363 |
|
|
|
| 2 |
C |
-0.363 |
|
|
|
| 3 |
Br |
-0.058 |
|
|
|
| 4 |
Br |
-0.058 |
|
|
|
| 5 |
H |
0.189 |
|
|
|
| 6 |
H |
0.232 |
|
|
|
| 7 |
H |
0.189 |
|
|
|
| 8 |
H |
0.232 |
|
|
|
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 |
2.596 |
2.596 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.411 |
0.964 |
0.000 |
| y |
0.964 |
-54.042 |
0.000 |
| z |
0.000 |
0.000 |
-45.206 |
|
| Traceless |
| | x | y | z |
| x |
0.213 |
0.964 |
0.000 |
| y |
0.964 |
-6.733 |
0.000 |
| z |
0.000 |
0.000 |
6.520 |
|
| Polar |
| 3z2-r2 | 13.040 |
| x2-y2 | 4.631 |
| xy | 0.964 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.712 |
-0.651 |
0.000 |
| y |
-0.651 |
12.012 |
0.000 |
| z |
0.000 |
0.000 |
10.210 |
<r2> (average value of r
2) Å
2
| <r2> |
311.661 |
| (<r2>)1/2 |
17.654 |