Jump to
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -5222.352418 |
| Energy at 298.15K | -5222.362563 |
| HF Energy | -5222.352418 |
| Nuclear repulsion energy | 413.735370 |
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 B1B95/6-31G
| 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 |
3175 |
3028 |
0.00 |
|
|
|
| 2 |
Ag |
1530 |
1459 |
0.00 |
|
|
|
| 3 |
Ag |
1314 |
1253 |
0.00 |
|
|
|
| 4 |
Ag |
1119 |
1068 |
0.00 |
|
|
|
| 5 |
Ag |
654 |
624 |
0.00 |
|
|
|
| 6 |
Ag |
188 |
180 |
0.00 |
|
|
|
| 7 |
Au |
3275 |
3123 |
1.23 |
|
|
|
| 8 |
Au |
1124 |
1072 |
2.83 |
|
|
|
| 9 |
Au |
777 |
741 |
8.29 |
|
|
|
| 10 |
Au |
104 |
99 |
5.44 |
|
|
|
| 11 |
Bg |
3251 |
3101 |
0.00 |
|
|
|
| 12 |
Bg |
1323 |
1262 |
0.00 |
|
|
|
| 13 |
Bg |
943 |
899 |
0.00 |
|
|
|
| 14 |
Bu |
3183 |
3035 |
5.12 |
|
|
|
| 15 |
Bu |
1523 |
1453 |
16.26 |
|
|
|
| 16 |
Bu |
1250 |
1192 |
46.04 |
|
|
|
| 17 |
Bu |
587 |
560 |
82.43 |
|
|
|
| 18 |
Bu |
178 |
170 |
8.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12749.6 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 12159.3 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 B1B95/6-31G
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.503 |
0.554 |
0.000 |
| C2 |
-0.503 |
-0.554 |
0.000 |
| Br3 |
-0.503 |
2.280 |
0.000 |
| Br4 |
0.503 |
-2.280 |
0.000 |
| H5 |
1.119 |
0.565 |
0.894 |
| H6 |
1.119 |
0.565 |
-0.894 |
| H7 |
-1.119 |
-0.565 |
0.894 |
| H8 |
-1.119 |
-0.565 |
-0.894 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4975 | 1.9984 | 2.8346 | 1.0858 | 1.0858 | 2.1643 | 2.1643 |
C2 | 1.4975 | | 2.8346 | 1.9984 | 2.1643 | 2.1643 | 1.0858 | 1.0858 | Br3 | 1.9984 | 2.8346 | | 4.6705 | 2.5249 | 2.5249 | 3.0452 | 3.0452 | Br4 | 2.8346 | 1.9984 | 4.6705 | | 3.0452 | 3.0452 | 2.5249 | 2.5249 | H5 | 1.0858 | 2.1643 | 2.5249 | 3.0452 | | 1.7888 | 2.5067 | 3.0795 | H6 | 1.0858 | 2.1643 | 2.5249 | 3.0452 | 1.7888 | | 3.0795 | 2.5067 | H7 | 2.1643 | 1.0858 | 3.0452 | 2.5249 | 2.5067 | 3.0795 | | 1.7888 | H8 | 2.1643 | 1.0858 | 3.0452 | 2.5249 | 3.0795 | 2.5067 | 1.7888 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
107.492 |
|
C1 |
C2 |
H7 |
112.851 |
| C1 |
C2 |
H8 |
112.851 |
|
C2 |
C1 |
Br3 |
107.492 |
| C2 |
C1 |
H5 |
112.851 |
|
C2 |
C1 |
H6 |
112.851 |
| Br3 |
C1 |
H5 |
106.095 |
|
Br3 |
C1 |
H6 |
106.095 |
| Br4 |
C2 |
H7 |
106.095 |
|
Br4 |
C2 |
H8 |
106.095 |
| H5 |
C1 |
H6 |
110.926 |
|
H7 |
C2 |
H8 |
110.926 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.516 |
|
|
|
| 2 |
C |
-0.516 |
|
|
|
| 3 |
Br |
0.019 |
|
|
|
| 4 |
Br |
0.019 |
|
|
|
| 5 |
H |
0.248 |
|
|
|
| 6 |
H |
0.248 |
|
|
|
| 7 |
H |
0.248 |
|
|
|
| 8 |
H |
0.248 |
|
|
|
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 |
-48.468 |
1.915 |
0.000 |
| y |
1.915 |
-57.133 |
0.000 |
| z |
0.000 |
0.000 |
-49.058 |
|
| Traceless |
| | x | y | z |
| x |
4.627 |
1.915 |
0.000 |
| y |
1.915 |
-8.369 |
0.000 |
| z |
0.000 |
0.000 |
3.742 |
|
| Polar |
| 3z2-r2 | 7.484 |
| x2-y2 | 8.664 |
| xy | 1.915 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.308 |
-2.688 |
0.000 |
| y |
-2.688 |
11.558 |
0.000 |
| z |
0.000 |
0.000 |
3.858 |
<r2> (average value of r
2) Å
2
| <r2> |
430.153 |
| (<r2>)1/2 |
20.740 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -5222.348973 |
| Energy at 298.15K | |
| HF Energy | -5222.348973 |
| Nuclear repulsion energy | 455.340804 |
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 B1B95/6-31G
| 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 |
3228 |
3078 |
0.03 |
112.43 |
0.75 |
0.85 |
| 2 |
A |
3153 |
3007 |
11.35 |
234.91 |
0.01 |
0.02 |
| 3 |
A |
1508 |
1439 |
1.32 |
8.30 |
0.70 |
0.82 |
| 4 |
A |
1342 |
1280 |
21.13 |
6.26 |
0.63 |
0.77 |
| 5 |
A |
1217 |
1161 |
1.37 |
32.01 |
0.74 |
0.85 |
| 6 |
A |
1080 |
1030 |
2.12 |
4.84 |
0.62 |
0.77 |
| 7 |
A |
925 |
882 |
8.82 |
16.81 |
0.57 |
0.73 |
| 8 |
A |
549 |
523 |
12.07 |
20.70 |
0.12 |
0.21 |
| 9 |
A |
227 |
217 |
1.15 |
1.73 |
0.54 |
0.70 |
| 10 |
A |
86 |
82 |
0.21 |
1.92 |
0.74 |
0.85 |
| 11 |
B |
3242 |
3092 |
1.55 |
37.79 |
0.75 |
0.86 |
| 12 |
B |
3146 |
3000 |
1.99 |
63.11 |
0.75 |
0.86 |
| 13 |
B |
1505 |
1435 |
19.04 |
22.75 |
0.75 |
0.86 |
| 14 |
B |
1314 |
1253 |
45.58 |
2.28 |
0.75 |
0.86 |
| 15 |
B |
1149 |
1096 |
2.18 |
11.80 |
0.75 |
0.86 |
| 16 |
B |
859 |
819 |
23.86 |
1.19 |
0.75 |
0.86 |
| 17 |
B |
582 |
555 |
15.39 |
15.13 |
0.75 |
0.86 |
| 18 |
B |
358 |
341 |
9.13 |
5.32 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12734.6 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 12145.0 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 B1B95/6-31G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.312 |
0.682 |
1.249 |
| C2 |
-0.312 |
-0.682 |
1.249 |
| Br3 |
-0.312 |
1.742 |
-0.308 |
| Br4 |
0.312 |
-1.742 |
-0.308 |
| H5 |
0.010 |
1.249 |
2.128 |
| H6 |
1.395 |
0.645 |
1.172 |
| H7 |
-0.010 |
-1.249 |
2.128 |
| H8 |
-1.395 |
-0.645 |
1.172 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4988 | 1.9845 | 2.8809 | 1.0890 | 1.0865 | 2.1457 | 2.1626 |
C2 | 1.4988 | | 2.8809 | 1.9845 | 2.1457 | 2.1626 | 1.0890 | 1.0865 | Br3 | 1.9845 | 2.8809 | | 3.5400 | 2.5060 | 2.5116 | 3.8698 | 3.0105 | Br4 | 2.8809 | 1.9845 | 3.5400 | | 3.8698 | 3.0105 | 2.5060 | 2.5116 | H5 | 1.0890 | 2.1457 | 2.5060 | 3.8698 | | 1.7880 | 2.4987 | 2.5442 | H6 | 1.0865 | 2.1626 | 2.5116 | 3.0105 | 1.7880 | | 2.5442 | 3.0732 | H7 | 2.1457 | 1.0890 | 3.8698 | 2.5060 | 2.4987 | 2.5442 | | 1.7880 | H8 | 2.1626 | 1.0865 | 3.0105 | 2.5116 | 2.5442 | 3.0732 | 1.7880 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
110.827 |
|
C1 |
C2 |
H7 |
111.030 |
| C1 |
C2 |
H8 |
112.567 |
|
C2 |
C1 |
Br3 |
110.827 |
| C2 |
C1 |
H5 |
111.030 |
|
C2 |
C1 |
H6 |
112.567 |
| Br3 |
C1 |
H5 |
105.513 |
|
Br3 |
C1 |
H6 |
106.013 |
| Br4 |
C2 |
H7 |
105.513 |
|
Br4 |
C2 |
H8 |
106.013 |
| H5 |
C1 |
H6 |
110.545 |
|
H7 |
C2 |
H8 |
110.545 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.524 |
|
|
|
| 2 |
C |
-0.524 |
|
|
|
| 3 |
Br |
0.038 |
|
|
|
| 4 |
Br |
0.038 |
|
|
|
| 5 |
H |
0.238 |
|
|
|
| 6 |
H |
0.247 |
|
|
|
| 7 |
H |
0.238 |
|
|
|
| 8 |
H |
0.247 |
|
|
|
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 |
3.069 |
3.069 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.833 |
1.110 |
0.000 |
| y |
1.110 |
-53.635 |
0.000 |
| z |
0.000 |
0.000 |
-44.485 |
|
| Traceless |
| | x | y | z |
| x |
0.227 |
1.110 |
0.000 |
| y |
1.110 |
-6.976 |
0.000 |
| z |
0.000 |
0.000 |
6.749 |
|
| Polar |
| 3z2-r2 | 13.498 |
| x2-y2 | 4.802 |
| xy | 1.110 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.419 |
-1.012 |
0.000 |
| y |
-1.012 |
7.280 |
0.000 |
| z |
0.000 |
0.000 |
7.374 |
<r2> (average value of r
2) Å
2
| <r2> |
301.653 |
| (<r2>)1/2 |
17.368 |