Jump to
S1C2
Energy calculated at TPSSh/STO-3G
| | hartrees |
| Energy at 0K | -5169.675282 |
| Energy at 298.15K | |
| HF Energy | -5169.675282 |
| Nuclear repulsion energy | 413.953832 |
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 TPSSh/STO-3G
| 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 |
3336 |
3336 |
0.00 |
77.70 |
0.10 |
0.19 |
| 2 |
Ag |
1645 |
1645 |
0.00 |
25.07 |
0.75 |
0.86 |
| 3 |
Ag |
1427 |
1427 |
0.00 |
14.77 |
0.31 |
0.48 |
| 4 |
Ag |
1094 |
1094 |
0.00 |
11.39 |
0.74 |
0.85 |
| 5 |
Ag |
792 |
792 |
0.00 |
35.83 |
0.31 |
0.47 |
| 6 |
Ag |
202 |
202 |
0.00 |
3.56 |
0.40 |
0.57 |
| 7 |
Au |
3462 |
3462 |
1.06 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1215 |
1215 |
0.22 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
787 |
787 |
2.93 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
88 |
88 |
3.19 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3447 |
3447 |
0.00 |
57.92 |
0.75 |
0.86 |
| 12 |
Bg |
1395 |
1395 |
0.00 |
18.30 |
0.75 |
0.86 |
| 13 |
Bg |
1018 |
1018 |
0.00 |
9.25 |
0.75 |
0.86 |
| 14 |
Bu |
3343 |
3343 |
2.32 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1656 |
1656 |
1.55 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1328 |
1328 |
44.79 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
733 |
733 |
31.47 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
177 |
177 |
5.07 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13572.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13572.4 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 TPSSh/STO-3G
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.488 |
0.608 |
0.000 |
| C2 |
-0.488 |
-0.608 |
0.000 |
| Br3 |
-0.488 |
2.288 |
0.000 |
| Br4 |
0.488 |
-2.288 |
0.000 |
| H5 |
1.134 |
0.576 |
0.897 |
| H6 |
1.134 |
0.576 |
-0.897 |
| H7 |
-1.134 |
-0.576 |
0.897 |
| H8 |
-1.134 |
-0.576 |
-0.897 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5582 | 1.9435 | 2.8959 | 1.1056 | 1.1056 | 2.1989 | 2.1989 |
C2 | 1.5582 | | 2.8959 | 1.9435 | 2.1989 | 2.1989 | 1.1056 | 1.1056 | Br3 | 1.9435 | 2.8959 | | 4.6797 | 2.5232 | 2.5232 | 3.0703 | 3.0703 | Br4 | 2.8959 | 1.9435 | 4.6797 | | 3.0703 | 3.0703 | 2.5232 | 2.5232 | H5 | 1.1056 | 2.1989 | 2.5232 | 3.0703 | | 1.7930 | 2.5440 | 3.1124 | H6 | 1.1056 | 2.1989 | 2.5232 | 3.0703 | 1.7930 | | 3.1124 | 2.5440 | H7 | 2.1989 | 1.1056 | 3.0703 | 2.5232 | 2.5440 | 3.1124 | | 1.7930 | H8 | 2.1989 | 1.1056 | 3.0703 | 2.5232 | 3.1124 | 2.5440 | 1.7930 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
111.107 |
|
C1 |
C2 |
H7 |
110.108 |
| C1 |
C2 |
H8 |
110.108 |
|
C2 |
C1 |
Br3 |
111.107 |
| C2 |
C1 |
H5 |
110.108 |
|
C2 |
C1 |
H6 |
110.108 |
| Br3 |
C1 |
H5 |
108.545 |
|
Br3 |
C1 |
H6 |
108.545 |
| Br4 |
C2 |
H7 |
108.545 |
|
Br4 |
C2 |
H8 |
108.545 |
| H5 |
C1 |
H6 |
108.359 |
|
H7 |
C2 |
H8 |
108.359 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.167 |
|
|
|
| 2 |
C |
-0.167 |
|
|
|
| 3 |
Br |
-0.021 |
|
|
|
| 4 |
Br |
-0.021 |
|
|
|
| 5 |
H |
0.094 |
|
|
|
| 6 |
H |
0.094 |
|
|
|
| 7 |
H |
0.094 |
|
|
|
| 8 |
H |
0.094 |
|
|
|
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
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.601 |
-1.756 |
0.000 |
| y |
-1.756 |
5.971 |
0.000 |
| z |
0.000 |
0.000 |
1.732 |
<r2> (average value of r
2) Å
2
| <r2> |
429.534 |
| (<r2>)1/2 |
20.725 |
Jump to
S1C1
Energy calculated at TPSSh/STO-3G
| | hartrees |
| Energy at 0K | -5169.673029 |
| Energy at 298.15K | |
| HF Energy | -5169.673029 |
| Nuclear repulsion energy | 449.367237 |
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 TPSSh/STO-3G
| 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 |
3438 |
3438 |
0.07 |
57.36 |
0.74 |
0.85 |
| 2 |
A |
3327 |
3327 |
0.67 |
91.76 |
0.04 |
0.07 |
| 3 |
A |
1643 |
1643 |
0.65 |
8.05 |
0.72 |
0.84 |
| 4 |
A |
1435 |
1435 |
14.57 |
7.88 |
0.61 |
0.76 |
| 5 |
A |
1291 |
1291 |
0.02 |
17.60 |
0.75 |
0.85 |
| 6 |
A |
1089 |
1089 |
1.26 |
3.82 |
0.75 |
0.85 |
| 7 |
A |
993 |
993 |
4.29 |
5.97 |
0.58 |
0.73 |
| 8 |
A |
656 |
656 |
3.74 |
13.31 |
0.11 |
0.20 |
| 9 |
A |
214 |
214 |
0.66 |
1.15 |
0.44 |
0.61 |
| 10 |
A |
71 |
71 |
0.32 |
1.04 |
0.74 |
0.85 |
| 11 |
B |
3446 |
3446 |
0.91 |
20.79 |
0.75 |
0.86 |
| 12 |
B |
3326 |
3326 |
0.68 |
20.54 |
0.75 |
0.86 |
| 13 |
B |
1634 |
1634 |
1.83 |
22.84 |
0.75 |
0.86 |
| 14 |
B |
1415 |
1415 |
58.11 |
1.12 |
0.75 |
0.86 |
| 15 |
B |
1229 |
1229 |
0.44 |
7.25 |
0.75 |
0.86 |
| 16 |
B |
915 |
915 |
7.68 |
1.04 |
0.75 |
0.86 |
| 17 |
B |
701 |
701 |
5.05 |
9.51 |
0.75 |
0.86 |
| 18 |
B |
373 |
373 |
3.80 |
2.92 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13597.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13597.6 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 TPSSh/STO-3G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.295 |
0.723 |
1.197 |
| C2 |
-0.295 |
-0.723 |
1.197 |
| Br3 |
-0.295 |
1.804 |
-0.300 |
| Br4 |
0.295 |
-1.804 |
-0.300 |
| H5 |
-0.021 |
1.225 |
2.133 |
| H6 |
1.400 |
0.679 |
1.187 |
| H7 |
0.021 |
-1.225 |
2.133 |
| H8 |
-1.400 |
-0.679 |
1.187 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5615 | 1.9387 | 2.9374 | 1.1072 | 1.1058 | 2.1777 | 2.1994 |
C2 | 1.5615 | | 2.9374 | 1.9387 | 2.1777 | 2.1994 | 1.1072 | 1.1058 | Br3 | 1.9387 | 2.9374 | | 3.6562 | 2.5157 | 2.5194 | 3.8975 | 3.0982 | Br4 | 2.9374 | 1.9387 | 3.6562 | | 3.8975 | 3.0982 | 2.5157 | 2.5194 | H5 | 1.1072 | 2.1777 | 2.5157 | 3.8975 | | 1.7916 | 2.4494 | 2.5337 | H6 | 1.1058 | 2.1994 | 2.5194 | 3.0982 | 1.7916 | | 2.5337 | 3.1116 | H7 | 2.1777 | 1.1072 | 3.8975 | 2.5157 | 2.4494 | 2.5337 | | 1.7916 | H8 | 2.1994 | 1.1058 | 3.0982 | 2.5194 | 2.5337 | 3.1116 | 1.7916 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.677 |
|
C1 |
C2 |
H7 |
108.167 |
| C1 |
C2 |
H8 |
109.920 |
|
C2 |
C1 |
Br3 |
113.677 |
| C2 |
C1 |
H5 |
108.167 |
|
C2 |
C1 |
H6 |
109.920 |
| Br3 |
C1 |
H5 |
108.243 |
|
Br3 |
C1 |
H6 |
108.573 |
| Br4 |
C2 |
H7 |
108.243 |
|
Br4 |
C2 |
H8 |
108.573 |
| H5 |
C1 |
H6 |
108.110 |
|
H7 |
C2 |
H8 |
108.110 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.169 |
|
|
|
| 2 |
C |
-0.169 |
|
|
|
| 3 |
Br |
-0.016 |
|
|
|
| 4 |
Br |
-0.016 |
|
|
|
| 5 |
H |
0.092 |
|
|
|
| 6 |
H |
0.094 |
|
|
|
| 7 |
H |
0.092 |
|
|
|
| 8 |
H |
0.094 |
|
|
|
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 |
2.172 |
2.172 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.044 |
-0.683 |
0.000 |
| y |
-0.683 |
3.683 |
0.000 |
| z |
0.000 |
0.000 |
3.921 |
<r2> (average value of r
2) Å
2
| <r2> |
312.769 |
| (<r2>)1/2 |
17.685 |