Jump to
S1C2
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -5169.669288 |
| Energy at 298.15K | -5169.679381 |
| HF Energy | -5169.669288 |
| Nuclear repulsion energy | 413.428083 |
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 B3LYP/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 |
3332 |
2974 |
0.00 |
|
|
|
| 2 |
Ag |
1641 |
1464 |
0.00 |
|
|
|
| 3 |
Ag |
1432 |
1278 |
0.00 |
|
|
|
| 4 |
Ag |
1091 |
973 |
0.00 |
|
|
|
| 5 |
Ag |
792 |
706 |
0.00 |
|
|
|
| 6 |
Ag |
202 |
180 |
0.00 |
|
|
|
| 7 |
Au |
3458 |
3086 |
1.02 |
|
|
|
| 8 |
Au |
1220 |
1089 |
0.18 |
|
|
|
| 9 |
Au |
793 |
708 |
3.40 |
|
|
|
| 10 |
Au |
97 |
86 |
3.13 |
|
|
|
| 11 |
Bg |
3443 |
3073 |
0.00 |
|
|
|
| 12 |
Bg |
1395 |
1245 |
0.00 |
|
|
|
| 13 |
Bg |
1020 |
910 |
0.00 |
|
|
|
| 14 |
Bu |
3340 |
2980 |
2.38 |
|
|
|
| 15 |
Bu |
1652 |
1474 |
2.47 |
|
|
|
| 16 |
Bu |
1333 |
1190 |
40.07 |
|
|
|
| 17 |
Bu |
726 |
648 |
30.30 |
|
|
|
| 18 |
Bu |
184 |
164 |
4.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13574.7 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 12114.0 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 B3LYP/STO-3G
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.487 |
0.609 |
0.000 |
| C2 |
-0.487 |
-0.609 |
0.000 |
| Br3 |
-0.487 |
2.293 |
0.000 |
| Br4 |
0.487 |
-2.293 |
0.000 |
| H5 |
1.134 |
0.576 |
0.895 |
| H6 |
1.134 |
0.576 |
-0.895 |
| H7 |
-1.134 |
-0.576 |
0.895 |
| H8 |
-1.134 |
-0.576 |
-0.895 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5595 | 1.9452 | 2.9015 | 1.1048 | 1.1048 | 2.1986 | 2.1986 |
C2 | 1.5595 | | 2.9015 | 1.9452 | 2.1986 | 2.1986 | 1.1048 | 1.1048 | Br3 | 1.9452 | 2.9015 | | 4.6875 | 2.5249 | 2.5249 | 3.0741 | 3.0741 | Br4 | 2.9015 | 1.9452 | 4.6875 | | 3.0741 | 3.0741 | 2.5249 | 2.5249 | H5 | 1.1048 | 2.1986 | 2.5249 | 3.0741 | | 1.7897 | 2.5443 | 3.1107 | H6 | 1.1048 | 2.1986 | 2.5249 | 3.0741 | 1.7897 | | 3.1107 | 2.5443 | H7 | 2.1986 | 1.1048 | 3.0741 | 2.5249 | 2.5443 | 3.1107 | | 1.7897 | H8 | 2.1986 | 1.1048 | 3.0741 | 2.5249 | 3.1107 | 2.5443 | 1.7897 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
111.289 |
|
C1 |
C2 |
H7 |
110.047 |
| C1 |
C2 |
H8 |
110.047 |
|
C2 |
C1 |
Br3 |
111.289 |
| C2 |
C1 |
H5 |
110.047 |
|
C2 |
C1 |
H6 |
110.047 |
| Br3 |
C1 |
H5 |
108.596 |
|
Br3 |
C1 |
H6 |
108.596 |
| Br4 |
C2 |
H7 |
108.596 |
|
Br4 |
C2 |
H8 |
108.596 |
| H5 |
C1 |
H6 |
108.190 |
|
H7 |
C2 |
H8 |
108.190 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.180 |
|
|
|
| 2 |
C |
-0.180 |
|
|
|
| 3 |
Br |
-0.016 |
|
|
|
| 4 |
Br |
-0.016 |
|
|
|
| 5 |
H |
0.098 |
|
|
|
| 6 |
H |
0.098 |
|
|
|
| 7 |
H |
0.098 |
|
|
|
| 8 |
H |
0.098 |
|
|
|
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 |
-44.649 |
1.558 |
0.000 |
| y |
1.558 |
-51.150 |
0.000 |
| z |
0.000 |
0.000 |
-44.817 |
|
| Traceless |
| | x | y | z |
| x |
3.335 |
1.558 |
0.000 |
| y |
1.558 |
-6.417 |
0.000 |
| z |
0.000 |
0.000 |
3.082 |
|
| Polar |
| 3z2-r2 | 6.164 |
| x2-y2 | 6.501 |
| xy | 1.558 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.606 |
-1.767 |
0.000 |
| y |
-1.767 |
5.964 |
0.000 |
| z |
0.000 |
0.000 |
1.728 |
<r2> (average value of r
2) Å
2
| <r2> |
430.770 |
| (<r2>)1/2 |
20.755 |
Jump to
S1C1
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -5169.667171 |
| Energy at 298.15K | |
| HF Energy | -5169.667171 |
| Nuclear repulsion energy | 449.254694 |
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 B3LYP/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 |
3433 |
3063 |
0.06 |
56.72 |
0.74 |
0.85 |
| 2 |
A |
3322 |
2965 |
0.74 |
89.26 |
0.04 |
0.07 |
| 3 |
A |
1638 |
1462 |
0.29 |
7.97 |
0.73 |
0.85 |
| 4 |
A |
1436 |
1282 |
13.35 |
7.46 |
0.59 |
0.74 |
| 5 |
A |
1295 |
1155 |
0.00 |
17.56 |
0.75 |
0.85 |
| 6 |
A |
1087 |
970 |
1.23 |
3.70 |
0.75 |
0.85 |
| 7 |
A |
995 |
888 |
4.54 |
5.91 |
0.58 |
0.73 |
| 8 |
A |
655 |
584 |
3.72 |
13.61 |
0.11 |
0.20 |
| 9 |
A |
215 |
192 |
0.68 |
1.14 |
0.45 |
0.62 |
| 10 |
A |
72 |
64 |
0.32 |
1.07 |
0.74 |
0.85 |
| 11 |
B |
3441 |
3071 |
0.83 |
20.63 |
0.75 |
0.86 |
| 12 |
B |
3321 |
2964 |
0.78 |
20.12 |
0.75 |
0.86 |
| 13 |
B |
1631 |
1455 |
2.76 |
22.60 |
0.75 |
0.86 |
| 14 |
B |
1418 |
1266 |
52.21 |
0.86 |
0.75 |
0.86 |
| 15 |
B |
1233 |
1100 |
0.37 |
7.18 |
0.75 |
0.86 |
| 16 |
B |
918 |
819 |
8.05 |
1.07 |
0.75 |
0.86 |
| 17 |
B |
700 |
625 |
5.04 |
9.74 |
0.75 |
0.86 |
| 18 |
B |
375 |
335 |
3.77 |
2.97 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13592.3 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 12129.7 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 B3LYP/STO-3G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.295 |
0.723 |
1.201 |
| C2 |
-0.295 |
-0.723 |
1.201 |
| Br3 |
-0.295 |
1.803 |
-0.301 |
| Br4 |
0.295 |
-1.803 |
-0.301 |
| H5 |
-0.018 |
1.226 |
2.135 |
| H6 |
1.399 |
0.678 |
1.190 |
| H7 |
0.018 |
-1.226 |
2.135 |
| H8 |
-1.399 |
-0.678 |
1.190 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5623 | 1.9413 | 2.9387 | 1.1063 | 1.1049 | 2.1792 | 2.1991 |
C2 | 1.5623 | | 2.9387 | 1.9413 | 2.1792 | 2.1991 | 1.1063 | 1.1049 | Br3 | 1.9413 | 2.9387 | | 3.6541 | 2.5182 | 2.5216 | 3.8994 | 3.0982 | Br4 | 2.9387 | 1.9413 | 3.6541 | | 3.8994 | 3.0982 | 2.5182 | 2.5216 | H5 | 1.1063 | 2.1792 | 2.5182 | 3.8994 | | 1.7892 | 2.4523 | 2.5350 | H6 | 1.1049 | 2.1991 | 2.5216 | 3.0982 | 1.7892 | | 2.5350 | 3.1100 | H7 | 2.1792 | 1.1063 | 3.8994 | 2.5182 | 2.4523 | 2.5350 | | 1.7892 | H8 | 2.1991 | 1.1049 | 3.0982 | 2.5216 | 2.5350 | 3.1100 | 1.7892 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.577 |
|
C1 |
C2 |
H7 |
108.281 |
| C1 |
C2 |
H8 |
109.885 |
|
C2 |
C1 |
Br3 |
113.577 |
| C2 |
C1 |
H5 |
108.281 |
|
C2 |
C1 |
H6 |
109.885 |
| Br3 |
C1 |
H5 |
108.303 |
|
Br3 |
C1 |
H6 |
108.611 |
| Br4 |
C2 |
H7 |
108.303 |
|
Br4 |
C2 |
H8 |
108.611 |
| H5 |
C1 |
H6 |
108.034 |
|
H7 |
C2 |
H8 |
108.034 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.182 |
|
|
|
| 2 |
C |
-0.182 |
|
|
|
| 3 |
Br |
-0.013 |
|
|
|
| 4 |
Br |
-0.013 |
|
|
|
| 5 |
H |
0.096 |
|
|
|
| 6 |
H |
0.098 |
|
|
|
| 7 |
H |
0.096 |
|
|
|
| 8 |
H |
0.098 |
|
|
|
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 |
2.149 |
2.149 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-44.759 |
0.843 |
0.000 |
| y |
0.843 |
-48.486 |
0.000 |
| z |
0.000 |
0.000 |
-42.294 |
|
| Traceless |
| | x | y | z |
| x |
0.631 |
0.843 |
0.000 |
| y |
0.843 |
-4.960 |
0.000 |
| z |
0.000 |
0.000 |
4.328 |
|
| Polar |
| 3z2-r2 | 8.657 |
| x2-y2 | 3.727 |
| xy | 0.843 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.046 |
-0.690 |
0.000 |
| y |
-0.690 |
3.687 |
0.000 |
| z |
0.000 |
0.000 |
3.948 |
<r2> (average value of r
2) Å
2
| <r2> |
312.622 |
| (<r2>)1/2 |
17.681 |