Jump to
S1C2
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -5226.164824 |
| Energy at 298.15K | |
| HF Energy | -5226.164824 |
| Nuclear repulsion energy | 418.816111 |
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/6-311+G(3df,2p)
| 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 |
3116 |
3116 |
0.00 |
151.36 |
0.02 |
0.05 |
| 2 |
Ag |
1484 |
1484 |
0.00 |
5.92 |
0.72 |
0.84 |
| 3 |
Ag |
1280 |
1280 |
0.00 |
48.24 |
0.29 |
0.45 |
| 4 |
Ag |
1085 |
1085 |
0.00 |
8.04 |
0.73 |
0.84 |
| 5 |
Ag |
681 |
681 |
0.00 |
100.80 |
0.25 |
0.40 |
| 6 |
Ag |
192 |
192 |
0.00 |
4.25 |
0.21 |
0.34 |
| 7 |
Au |
3201 |
3201 |
0.03 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1103 |
1103 |
2.49 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
756 |
756 |
3.73 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
103 |
103 |
4.38 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3177 |
3177 |
0.00 |
71.03 |
0.75 |
0.86 |
| 12 |
Bg |
1285 |
1285 |
0.00 |
1.91 |
0.75 |
0.86 |
| 13 |
Bg |
946 |
946 |
0.00 |
0.89 |
0.75 |
0.86 |
| 14 |
Bu |
3124 |
3124 |
4.05 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1479 |
1479 |
9.17 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1206 |
1206 |
45.39 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
613 |
613 |
70.36 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
179 |
179 |
6.71 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12504.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12504.3 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/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.491 |
0.568 |
0.000 |
| C2 |
-0.491 |
-0.568 |
0.000 |
| Br3 |
-0.491 |
2.256 |
0.000 |
| Br4 |
0.491 |
-2.256 |
0.000 |
| H5 |
1.113 |
0.574 |
0.890 |
| H6 |
1.113 |
0.574 |
-0.890 |
| H7 |
-1.113 |
-0.574 |
0.890 |
| H8 |
-1.113 |
-0.574 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5006 | 1.9526 | 2.8231 | 1.0859 | 1.0859 | 2.1606 | 2.1606 |
C2 | 1.5006 | | 2.8231 | 1.9526 | 2.1606 | 2.1606 | 1.0859 | 1.0859 | Br3 | 1.9526 | 2.8231 | | 4.6166 | 2.4880 | 2.4880 | 3.0311 | 3.0311 | Br4 | 2.8231 | 1.9526 | 4.6166 | | 3.0311 | 3.0311 | 2.4880 | 2.4880 | H5 | 1.0859 | 2.1606 | 2.4880 | 3.0311 | | 1.7799 | 2.5049 | 3.0729 | H6 | 1.0859 | 2.1606 | 2.4880 | 3.0311 | 1.7799 | | 3.0729 | 2.5049 | H7 | 2.1606 | 1.0859 | 3.0311 | 2.4880 | 2.5049 | 3.0729 | | 1.7799 | H8 | 2.1606 | 1.0859 | 3.0311 | 2.4880 | 3.0729 | 2.5049 | 1.7799 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.971 |
|
C1 |
C2 |
H7 |
112.307 |
| C1 |
C2 |
H8 |
112.307 |
|
C2 |
C1 |
Br3 |
108.971 |
| C2 |
C1 |
H5 |
112.307 |
|
C2 |
C1 |
H6 |
112.307 |
| Br3 |
C1 |
H5 |
106.413 |
|
Br3 |
C1 |
H6 |
106.413 |
| Br4 |
C2 |
H7 |
106.413 |
|
Br4 |
C2 |
H8 |
106.413 |
| H5 |
C1 |
H6 |
110.079 |
|
H7 |
C2 |
H8 |
110.079 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.270 |
|
|
|
| 2 |
C |
-0.270 |
|
|
|
| 3 |
Br |
-0.098 |
|
|
|
| 4 |
Br |
-0.098 |
|
|
|
| 5 |
H |
0.184 |
|
|
|
| 6 |
H |
0.184 |
|
|
|
| 7 |
H |
0.184 |
|
|
|
| 8 |
H |
0.184 |
|
|
|
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 |
-48.993 |
1.400 |
0.000 |
| y |
1.400 |
-55.895 |
0.000 |
| z |
0.000 |
0.000 |
-49.633 |
|
| Traceless |
| | x | y | z |
| x |
3.771 |
1.400 |
0.000 |
| y |
1.400 |
-6.582 |
0.000 |
| z |
0.000 |
0.000 |
2.811 |
|
| Polar |
| 3z2-r2 | 5.622 |
| x2-y2 | 6.902 |
| xy | 1.400 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.046 |
-1.664 |
0.000 |
| y |
-1.664 |
14.611 |
0.000 |
| z |
0.000 |
0.000 |
8.218 |
<r2> (average value of r
2) Å
2
| <r2> |
421.346 |
| (<r2>)1/2 |
20.527 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -5226.161453 |
| Energy at 298.15K | |
| HF Energy | -5226.161453 |
| Nuclear repulsion energy | 452.877428 |
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/6-311+G(3df,2p)
| 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 |
3157 |
3157 |
0.00 |
81.58 |
0.75 |
0.86 |
| 2 |
A |
3097 |
3097 |
12.10 |
243.89 |
0.02 |
0.04 |
| 3 |
A |
1460 |
1460 |
1.36 |
2.98 |
0.72 |
0.84 |
| 4 |
A |
1306 |
1306 |
16.46 |
5.18 |
0.14 |
0.25 |
| 5 |
A |
1195 |
1195 |
0.83 |
5.46 |
0.74 |
0.85 |
| 6 |
A |
1048 |
1048 |
1.22 |
1.33 |
0.51 |
0.68 |
| 7 |
A |
910 |
910 |
7.15 |
4.53 |
0.17 |
0.30 |
| 8 |
A |
573 |
573 |
6.78 |
21.61 |
0.05 |
0.09 |
| 9 |
A |
229 |
229 |
1.29 |
1.30 |
0.19 |
0.32 |
| 10 |
A |
78 |
78 |
0.22 |
0.70 |
0.62 |
0.76 |
| 11 |
B |
3171 |
3171 |
0.26 |
26.42 |
0.75 |
0.86 |
| 12 |
B |
3089 |
3089 |
1.90 |
38.95 |
0.75 |
0.86 |
| 13 |
B |
1457 |
1457 |
14.70 |
8.63 |
0.75 |
0.86 |
| 14 |
B |
1274 |
1274 |
58.79 |
3.57 |
0.75 |
0.86 |
| 15 |
B |
1124 |
1124 |
1.22 |
1.12 |
0.75 |
0.86 |
| 16 |
B |
849 |
849 |
18.78 |
1.01 |
0.75 |
0.86 |
| 17 |
B |
606 |
606 |
14.33 |
7.41 |
0.75 |
0.86 |
| 18 |
B |
359 |
359 |
5.97 |
1.67 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12491.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12491.7 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/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.308 |
0.685 |
1.176 |
| C2 |
-0.308 |
-0.685 |
1.176 |
| Br3 |
-0.308 |
1.797 |
-0.293 |
| Br4 |
0.308 |
-1.797 |
-0.293 |
| H5 |
0.026 |
1.213 |
2.085 |
| H6 |
1.392 |
0.645 |
1.099 |
| H7 |
-0.026 |
-1.213 |
2.085 |
| H8 |
-1.392 |
-0.645 |
1.099 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5015 | 1.9423 | 2.8829 | 1.0894 | 1.0866 | 2.1307 | 2.1595 |
C2 | 1.5015 | | 2.8829 | 1.9423 | 2.1307 | 2.1595 | 1.0894 | 1.0866 | Br3 | 1.9423 | 2.8829 | | 3.6456 | 2.4710 | 2.4804 | 3.8460 | 3.0120 | Br4 | 2.8829 | 1.9423 | 3.6456 | | 3.8460 | 3.0120 | 2.4710 | 2.4804 | H5 | 1.0894 | 2.1307 | 2.4710 | 3.8460 | | 1.7779 | 2.4267 | 2.5365 | H6 | 1.0866 | 2.1595 | 2.4804 | 3.0120 | 1.7779 | | 2.5365 | 3.0677 | H7 | 2.1307 | 1.0894 | 3.8460 | 2.4710 | 2.4267 | 2.5365 | | 1.7779 | H8 | 2.1595 | 1.0866 | 3.0120 | 2.4804 | 2.5365 | 3.0677 | 1.7779 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.054 |
|
C1 |
C2 |
H7 |
109.618 |
| C1 |
C2 |
H8 |
112.111 |
|
C2 |
C1 |
Br3 |
113.054 |
| C2 |
C1 |
H5 |
109.618 |
|
C2 |
C1 |
H6 |
112.111 |
| Br3 |
C1 |
H5 |
105.723 |
|
Br3 |
C1 |
H6 |
106.501 |
| Br4 |
C2 |
H7 |
105.723 |
|
Br4 |
C2 |
H8 |
106.501 |
| H5 |
C1 |
H6 |
109.579 |
|
H7 |
C2 |
H8 |
109.579 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.238 |
|
|
|
| 2 |
C |
-0.238 |
|
|
|
| 3 |
Br |
-0.099 |
|
|
|
| 4 |
Br |
-0.099 |
|
|
|
| 5 |
H |
0.163 |
|
|
|
| 6 |
H |
0.173 |
|
|
|
| 7 |
H |
0.163 |
|
|
|
| 8 |
H |
0.173 |
|
|
|
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 |
2.601 |
2.601 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.404 |
0.984 |
0.000 |
| y |
0.984 |
-54.014 |
0.000 |
| z |
0.000 |
0.000 |
-45.199 |
|
| Traceless |
| | x | y | z |
| x |
0.202 |
0.984 |
0.000 |
| y |
0.984 |
-6.713 |
0.000 |
| z |
0.000 |
0.000 |
6.510 |
|
| Polar |
| 3z2-r2 | 13.021 |
| x2-y2 | 4.610 |
| xy | 0.984 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.506 |
-0.676 |
0.000 |
| y |
-0.676 |
11.791 |
0.000 |
| z |
0.000 |
0.000 |
10.001 |
<r2> (average value of r
2) Å
2
| <r2> |
311.625 |
| (<r2>)1/2 |
17.653 |