Jump to
S1C2
Energy calculated at HF/6-31+G**
| | hartrees |
| Energy at 0K | -5217.886636 |
| Energy at 298.15K | -5217.897016 |
| HF Energy | -5217.886636 |
| Nuclear repulsion energy | 417.819354 |
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 HF/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 |
3290 |
2975 |
0.00 |
|
|
|
| 2 |
Ag |
1622 |
1466 |
0.00 |
|
|
|
| 3 |
Ag |
1437 |
1299 |
0.00 |
|
|
|
| 4 |
Ag |
1138 |
1029 |
0.00 |
|
|
|
| 5 |
Ag |
730 |
660 |
0.00 |
|
|
|
| 6 |
Ag |
206 |
186 |
0.00 |
|
|
|
| 7 |
Au |
3377 |
3054 |
0.14 |
|
|
|
| 8 |
Au |
1224 |
1106 |
3.25 |
|
|
|
| 9 |
Au |
820 |
741 |
2.83 |
|
|
|
| 10 |
Au |
135 |
122 |
6.55 |
|
|
|
| 11 |
Bg |
3355 |
3034 |
0.00 |
|
|
|
| 12 |
Bg |
1407 |
1272 |
0.00 |
|
|
|
| 13 |
Bg |
1050 |
949 |
0.00 |
|
|
|
| 14 |
Bu |
3296 |
2980 |
10.76 |
|
|
|
| 15 |
Bu |
1613 |
1459 |
9.13 |
|
|
|
| 16 |
Bu |
1346 |
1217 |
99.85 |
|
|
|
| 17 |
Bu |
638 |
577 |
106.59 |
|
|
|
| 18 |
Bu |
192 |
173 |
7.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13437.1 cm
-1
Scaled (by 0.9042) Zero Point Vibrational Energy (zpe) 12149.8 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 HF/6-31+G**
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.490 |
0.574 |
0.000 |
| C2 |
-0.490 |
-0.574 |
0.000 |
| Br3 |
-0.490 |
2.264 |
0.000 |
| Br4 |
0.490 |
-2.264 |
0.000 |
| H5 |
1.106 |
0.583 |
0.883 |
| H6 |
1.106 |
0.583 |
-0.883 |
| H7 |
-1.106 |
-0.583 |
0.883 |
| H8 |
-1.106 |
-0.583 |
-0.883 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5094 | 1.9536 | 2.8387 | 1.0769 | 1.0769 | 2.1598 | 2.1598 |
C2 | 1.5094 | | 2.8387 | 1.9536 | 2.1598 | 2.1598 | 1.0769 | 1.0769 | Br3 | 1.9536 | 2.8387 | | 4.6337 | 2.4809 | 2.4809 | 3.0440 | 3.0440 | Br4 | 2.8387 | 1.9536 | 4.6337 | | 3.0440 | 3.0440 | 2.4809 | 2.4809 | H5 | 1.0769 | 2.1598 | 2.4809 | 3.0440 | | 1.7662 | 2.5003 | 3.0612 | H6 | 1.0769 | 2.1598 | 2.4809 | 3.0440 | 1.7662 | | 3.0612 | 2.5003 | H7 | 2.1598 | 1.0769 | 3.0440 | 2.4809 | 2.5003 | 3.0612 | | 1.7662 | H8 | 2.1598 | 1.0769 | 3.0440 | 2.4809 | 3.0612 | 2.5003 | 1.7662 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.445 |
|
C1 |
C2 |
H7 |
112.169 |
| C1 |
C2 |
H8 |
112.169 |
|
C2 |
C1 |
Br3 |
109.445 |
| C2 |
C1 |
H5 |
112.169 |
|
C2 |
C1 |
H6 |
112.169 |
| Br3 |
C1 |
H5 |
106.270 |
|
Br3 |
C1 |
H6 |
106.270 |
| Br4 |
C2 |
H7 |
106.270 |
|
Br4 |
C2 |
H8 |
106.270 |
| H5 |
C1 |
H6 |
110.174 |
|
H7 |
C2 |
H8 |
110.174 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.168 |
|
|
|
| 2 |
C |
-0.168 |
|
|
|
| 3 |
Br |
-0.210 |
|
|
|
| 4 |
Br |
-0.210 |
|
|
|
| 5 |
H |
0.189 |
|
|
|
| 6 |
H |
0.189 |
|
|
|
| 7 |
H |
0.189 |
|
|
|
| 8 |
H |
0.189 |
|
|
|
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 |
-49.530 |
1.839 |
0.000 |
| y |
1.839 |
-58.287 |
0.000 |
| z |
0.000 |
0.000 |
-50.268 |
|
| Traceless |
| | x | y | z |
| x |
4.747 |
1.839 |
0.000 |
| y |
1.839 |
-8.388 |
0.000 |
| z |
0.000 |
0.000 |
3.640 |
|
| Polar |
| 3z2-r2 | 7.281 |
| x2-y2 | 8.757 |
| xy | 1.839 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.628 |
-1.883 |
0.000 |
| y |
-1.883 |
12.552 |
0.000 |
| z |
0.000 |
0.000 |
6.827 |
<r2> (average value of r
2) Å
2
| <r2> |
424.867 |
| (<r2>)1/2 |
20.612 |
Jump to
S1C1
Energy calculated at HF/6-31+G**
| | hartrees |
| Energy at 0K | -5217.883064 |
| Energy at 298.15K | |
| HF Energy | -5217.883064 |
| Nuclear repulsion energy | 448.781079 |
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 HF/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 |
3340 |
3020 |
0.00 |
91.48 |
0.75 |
0.86 |
| 2 |
A |
3272 |
2959 |
22.05 |
189.90 |
0.04 |
0.08 |
| 3 |
A |
1611 |
1457 |
0.09 |
5.73 |
0.69 |
0.82 |
| 4 |
A |
1449 |
1310 |
36.01 |
5.19 |
0.22 |
0.36 |
| 5 |
A |
1319 |
1193 |
1.85 |
9.58 |
0.72 |
0.84 |
| 6 |
A |
1124 |
1016 |
0.16 |
3.28 |
0.69 |
0.82 |
| 7 |
A |
991 |
896 |
9.50 |
6.92 |
0.27 |
0.42 |
| 8 |
A |
592 |
535 |
16.76 |
29.92 |
0.08 |
0.14 |
| 9 |
A |
257 |
232 |
1.61 |
1.64 |
0.18 |
0.31 |
| 10 |
A |
79 |
72 |
0.43 |
1.01 |
0.70 |
0.82 |
| 11 |
B |
3350 |
3029 |
0.76 |
20.83 |
0.75 |
0.86 |
| 12 |
B |
3261 |
2949 |
3.68 |
39.19 |
0.75 |
0.86 |
| 13 |
B |
1603 |
1449 |
11.65 |
12.68 |
0.75 |
0.86 |
| 14 |
B |
1415 |
1280 |
105.87 |
2.72 |
0.75 |
0.86 |
| 15 |
B |
1238 |
1120 |
3.07 |
2.48 |
0.75 |
0.86 |
| 16 |
B |
944 |
854 |
18.17 |
1.16 |
0.75 |
0.86 |
| 17 |
B |
627 |
567 |
30.60 |
17.15 |
0.75 |
0.86 |
| 18 |
B |
393 |
356 |
8.82 |
2.84 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13433.0 cm
-1
Scaled (by 0.9042) Zero Point Vibrational Energy (zpe) 12146.1 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 HF/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.328 |
0.681 |
1.145 |
| C2 |
-0.328 |
-0.681 |
1.145 |
| Br3 |
-0.328 |
1.832 |
-0.285 |
| Br4 |
0.328 |
-1.832 |
-0.285 |
| H5 |
0.085 |
1.197 |
2.063 |
| H6 |
1.397 |
0.619 |
1.031 |
| H7 |
-0.085 |
-1.197 |
2.063 |
| H8 |
-1.397 |
-0.619 |
1.031 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5106 | 1.9493 | 2.8908 | 1.0801 | 1.0773 | 2.1297 | 2.1624 |
C2 | 1.5106 | | 2.8908 | 1.9493 | 2.1297 | 2.1624 | 1.0801 | 1.0773 | Br3 | 1.9493 | 2.8908 | | 3.7218 | 2.4666 | 2.4854 | 3.8393 | 2.9799 | Br4 | 2.8908 | 1.9493 | 3.7218 | | 3.8393 | 2.9799 | 2.4666 | 2.4854 | H5 | 1.0801 | 2.1297 | 2.4666 | 3.8393 | | 1.7662 | 2.3992 | 2.5607 | H6 | 1.0773 | 2.1624 | 2.4854 | 2.9799 | 1.7662 | | 2.5607 | 3.0560 | H7 | 2.1297 | 1.0801 | 3.8393 | 2.4666 | 2.3992 | 2.5607 | | 1.7662 | H8 | 2.1624 | 1.0773 | 2.9799 | 2.4854 | 2.5607 | 3.0560 | 1.7662 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
112.726 |
|
C1 |
C2 |
H7 |
109.455 |
| C1 |
C2 |
H8 |
112.271 |
|
C2 |
C1 |
Br3 |
112.726 |
| C2 |
C1 |
H5 |
109.455 |
|
C2 |
C1 |
H6 |
112.271 |
| Br3 |
C1 |
H5 |
105.390 |
|
Br3 |
C1 |
H6 |
106.836 |
| Br4 |
C2 |
H7 |
105.390 |
|
Br4 |
C2 |
H8 |
106.836 |
| H5 |
C1 |
H6 |
109.907 |
|
H7 |
C2 |
H8 |
109.907 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.163 |
|
|
|
| 2 |
C |
-0.163 |
|
|
|
| 3 |
Br |
-0.201 |
|
|
|
| 4 |
Br |
-0.201 |
|
|
|
| 5 |
H |
0.175 |
|
|
|
| 6 |
H |
0.189 |
|
|
|
| 7 |
H |
0.175 |
|
|
|
| 8 |
H |
0.189 |
|
|
|
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 |
3.053 |
3.053 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.910 |
1.279 |
0.000 |
| y |
1.279 |
-55.833 |
0.000 |
| z |
0.000 |
0.000 |
-45.552 |
|
| Traceless |
| | x | y | z |
| x |
0.783 |
1.279 |
0.000 |
| y |
1.279 |
-8.102 |
0.000 |
| z |
0.000 |
0.000 |
7.319 |
|
| Polar |
| 3z2-r2 | 14.638 |
| x2-y2 | 5.923 |
| xy | 1.279 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.191 |
-0.876 |
0.000 |
| y |
-0.876 |
9.964 |
0.000 |
| z |
0.000 |
0.000 |
8.703 |
<r2> (average value of r
2) Å
2
| <r2> |
320.351 |
| (<r2>)1/2 |
17.898 |