Jump to
S1C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -5222.828329 |
| Energy at 298.15K | -5222.838670 |
| HF Energy | -5222.828329 |
| Nuclear repulsion energy | 416.997794 |
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/6-311G**
| 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 |
3272 |
2973 |
0.00 |
|
|
|
| 2 |
Ag |
1616 |
1468 |
0.00 |
|
|
|
| 3 |
Ag |
1426 |
1295 |
0.00 |
|
|
|
| 4 |
Ag |
1129 |
1025 |
0.00 |
|
|
|
| 5 |
Ag |
725 |
659 |
0.00 |
|
|
|
| 6 |
Ag |
203 |
185 |
0.00 |
|
|
|
| 7 |
Au |
3356 |
3049 |
2.23 |
|
|
|
| 8 |
Au |
1211 |
1101 |
4.18 |
|
|
|
| 9 |
Au |
814 |
739 |
3.97 |
|
|
|
| 10 |
Au |
111 |
100 |
5.96 |
|
|
|
| 11 |
Bg |
3334 |
3029 |
0.00 |
|
|
|
| 12 |
Bg |
1400 |
1272 |
0.00 |
|
|
|
| 13 |
Bg |
1039 |
944 |
0.00 |
|
|
|
| 14 |
Bu |
3277 |
2977 |
13.87 |
|
|
|
| 15 |
Bu |
1605 |
1458 |
8.16 |
|
|
|
| 16 |
Bu |
1335 |
1213 |
102.03 |
|
|
|
| 17 |
Bu |
634 |
576 |
105.23 |
|
|
|
| 18 |
Bu |
197 |
179 |
7.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13341.0 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 12120.3 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 HF/6-311G**
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.491 |
0.574 |
0.000 |
| C2 |
-0.491 |
-0.574 |
0.000 |
| Br3 |
-0.491 |
2.269 |
0.000 |
| Br4 |
0.491 |
-2.269 |
0.000 |
| H5 |
1.106 |
0.582 |
0.884 |
| H6 |
1.106 |
0.582 |
-0.884 |
| H7 |
-1.106 |
-0.582 |
0.884 |
| H8 |
-1.106 |
-0.582 |
-0.884 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5109 | 1.9585 | 2.8439 | 1.0768 | 1.0768 | 2.1605 | 2.1605 |
C2 | 1.5109 | | 2.8439 | 1.9585 | 2.1605 | 2.1605 | 1.0768 | 1.0768 | Br3 | 1.9585 | 2.8439 | | 4.6437 | 2.4852 | 2.4852 | 3.0481 | 3.0481 | Br4 | 2.8439 | 1.9585 | 4.6437 | | 3.0481 | 3.0481 | 2.4852 | 2.4852 | H5 | 1.0768 | 2.1605 | 2.4852 | 3.0481 | | 1.7671 | 2.4997 | 3.0613 | H6 | 1.0768 | 2.1605 | 2.4852 | 3.0481 | 1.7671 | | 3.0613 | 2.4997 | H7 | 2.1605 | 1.0768 | 3.0481 | 2.4852 | 2.4997 | 3.0613 | | 1.7671 | H8 | 2.1605 | 1.0768 | 3.0481 | 2.4852 | 3.0613 | 2.4997 | 1.7671 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.437 |
|
C1 |
C2 |
H7 |
112.125 |
| C1 |
C2 |
H8 |
112.125 |
|
C2 |
C1 |
Br3 |
109.437 |
| C2 |
C1 |
H5 |
112.125 |
|
C2 |
C1 |
H6 |
112.125 |
| Br3 |
C1 |
H5 |
106.266 |
|
Br3 |
C1 |
H6 |
106.266 |
| Br4 |
C2 |
H7 |
106.266 |
|
Br4 |
C2 |
H8 |
106.266 |
| H5 |
C1 |
H6 |
110.281 |
|
H7 |
C2 |
H8 |
110.281 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.229 |
|
|
|
| 2 |
C |
-0.229 |
|
|
|
| 3 |
Br |
-0.106 |
|
|
|
| 4 |
Br |
-0.106 |
|
|
|
| 5 |
H |
0.168 |
|
|
|
| 6 |
H |
0.168 |
|
|
|
| 7 |
H |
0.168 |
|
|
|
| 8 |
H |
0.168 |
|
|
|
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 |
-49.324 |
1.729 |
0.000 |
| y |
1.729 |
-57.867 |
0.000 |
| z |
0.000 |
0.000 |
-49.979 |
|
| Traceless |
| | x | y | z |
| x |
4.599 |
1.729 |
0.000 |
| y |
1.729 |
-8.215 |
0.000 |
| z |
0.000 |
0.000 |
3.616 |
|
| Polar |
| 3z2-r2 | 7.232 |
| x2-y2 | 8.542 |
| xy | 1.729 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.514 |
-2.205 |
0.000 |
| y |
-2.205 |
12.050 |
0.000 |
| z |
0.000 |
0.000 |
5.242 |
<r2> (average value of r
2) Å
2
| <r2> |
426.307 |
| (<r2>)1/2 |
20.647 |
Jump to
S1C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -5222.824139 |
| Energy at 298.15K | |
| HF Energy | -5222.824139 |
| Nuclear repulsion energy | 448.697562 |
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/6-311G**
| 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 |
3315 |
3012 |
0.20 |
100.01 |
0.75 |
0.86 |
| 2 |
A |
3254 |
2957 |
26.55 |
205.27 |
0.03 |
0.06 |
| 3 |
A |
1598 |
1452 |
0.15 |
5.67 |
0.55 |
0.71 |
| 4 |
A |
1439 |
1307 |
36.38 |
3.37 |
0.39 |
0.56 |
| 5 |
A |
1309 |
1189 |
2.57 |
10.95 |
0.75 |
0.86 |
| 6 |
A |
1109 |
1007 |
0.33 |
2.75 |
0.72 |
0.84 |
| 7 |
A |
986 |
895 |
10.16 |
7.73 |
0.43 |
0.60 |
| 8 |
A |
592 |
538 |
16.34 |
26.22 |
0.09 |
0.16 |
| 9 |
A |
243 |
221 |
1.40 |
1.78 |
0.45 |
0.62 |
| 10 |
A |
84 |
76 |
0.39 |
1.71 |
0.72 |
0.84 |
| 11 |
B |
3327 |
3023 |
3.47 |
24.52 |
0.75 |
0.86 |
| 12 |
B |
3243 |
2946 |
3.85 |
44.99 |
0.75 |
0.86 |
| 13 |
B |
1589 |
1444 |
9.38 |
12.97 |
0.75 |
0.86 |
| 14 |
B |
1407 |
1278 |
102.40 |
4.03 |
0.75 |
0.86 |
| 15 |
B |
1227 |
1115 |
3.73 |
4.74 |
0.75 |
0.86 |
| 16 |
B |
927 |
842 |
20.31 |
1.89 |
0.75 |
0.86 |
| 17 |
B |
629 |
572 |
28.45 |
18.84 |
0.75 |
0.86 |
| 18 |
B |
382 |
347 |
8.42 |
3.26 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13329.2 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 12109.6 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 HF/6-311G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.315 |
0.688 |
1.160 |
| C2 |
-0.315 |
-0.688 |
1.160 |
| Br3 |
-0.315 |
1.830 |
-0.289 |
| Br4 |
0.315 |
-1.830 |
-0.289 |
| H5 |
0.046 |
1.201 |
2.071 |
| H6 |
1.387 |
0.642 |
1.071 |
| H7 |
-0.046 |
-1.201 |
2.071 |
| H8 |
-1.387 |
-0.642 |
1.071 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5125 | 1.9488 | 2.9042 | 1.0802 | 1.0774 | 2.1282 | 2.1616 |
C2 | 1.5125 | | 2.9042 | 1.9488 | 2.1282 | 2.1616 | 1.0802 | 1.0774 | Br3 | 1.9488 | 2.9042 | | 3.7129 | 2.4684 | 2.4811 | 3.8507 | 3.0177 | Br4 | 2.9042 | 1.9488 | 3.7129 | | 3.8507 | 3.0177 | 2.4684 | 2.4811 | H5 | 1.0802 | 2.1282 | 2.4684 | 3.8507 | | 1.7646 | 2.4047 | 2.5402 | H6 | 1.0774 | 2.1616 | 2.4811 | 3.0177 | 1.7646 | | 2.5402 | 3.0573 | H7 | 2.1282 | 1.0802 | 3.8507 | 2.4684 | 2.4047 | 2.5402 | | 1.7646 | H8 | 2.1616 | 1.0774 | 3.0177 | 2.4811 | 2.5402 | 3.0573 | 1.7646 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.479 |
|
C1 |
C2 |
H7 |
109.202 |
| C1 |
C2 |
H8 |
112.062 |
|
C2 |
C1 |
Br3 |
113.479 |
| C2 |
C1 |
H5 |
109.202 |
|
C2 |
C1 |
H6 |
112.062 |
| Br3 |
C1 |
H5 |
105.543 |
|
Br3 |
C1 |
H6 |
106.563 |
| Br4 |
C2 |
H7 |
105.543 |
|
Br4 |
C2 |
H8 |
106.563 |
| H5 |
C1 |
H6 |
109.746 |
|
H7 |
C2 |
H8 |
109.746 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.231 |
|
|
|
| 2 |
C |
-0.231 |
|
|
|
| 3 |
Br |
-0.090 |
|
|
|
| 4 |
Br |
-0.090 |
|
|
|
| 5 |
H |
0.154 |
|
|
|
| 6 |
H |
0.167 |
|
|
|
| 7 |
H |
0.154 |
|
|
|
| 8 |
H |
0.167 |
|
|
|
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 |
2.995 |
2.995 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.695 |
1.108 |
0.000 |
| y |
1.108 |
-55.167 |
0.000 |
| z |
0.000 |
0.000 |
-45.424 |
|
| Traceless |
| | x | y | z |
| x |
0.601 |
1.108 |
0.000 |
| y |
1.108 |
-7.608 |
0.000 |
| z |
0.000 |
0.000 |
7.007 |
|
| Polar |
| 3z2-r2 | 14.014 |
| x2-y2 | 5.472 |
| xy | 1.108 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.757 |
-0.922 |
0.000 |
| y |
-0.922 |
8.903 |
0.000 |
| z |
0.000 |
0.000 |
7.944 |
<r2> (average value of r
2) Å
2
| <r2> |
319.806 |
| (<r2>)1/2 |
17.883 |