Jump to
S1C2
Energy calculated at B3LYP/3-21G*
| | hartrees |
| Energy at 0K | -5202.281805 |
| Energy at 298.15K | -5202.291985 |
| HF Energy | -5202.281805 |
| Nuclear repulsion energy | 414.717499 |
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/3-21G*
| 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 |
3129 |
3010 |
0.00 |
|
|
|
| 2 |
Ag |
1538 |
1479 |
0.00 |
|
|
|
| 3 |
Ag |
1314 |
1264 |
0.00 |
|
|
|
| 4 |
Ag |
1033 |
993 |
0.00 |
|
|
|
| 5 |
Ag |
677 |
651 |
0.00 |
|
|
|
| 6 |
Ag |
190 |
183 |
0.00 |
|
|
|
| 7 |
Au |
3214 |
3092 |
1.13 |
|
|
|
| 8 |
Au |
1139 |
1095 |
3.33 |
|
|
|
| 9 |
Au |
783 |
753 |
7.33 |
|
|
|
| 10 |
Au |
108 |
104 |
3.72 |
|
|
|
| 11 |
Bg |
3188 |
3067 |
0.00 |
|
|
|
| 12 |
Bg |
1330 |
1280 |
0.00 |
|
|
|
| 13 |
Bg |
952 |
916 |
0.00 |
|
|
|
| 14 |
Bu |
3138 |
3019 |
5.92 |
|
|
|
| 15 |
Bu |
1539 |
1481 |
11.52 |
|
|
|
| 16 |
Bu |
1248 |
1200 |
44.78 |
|
|
|
| 17 |
Bu |
609 |
586 |
66.69 |
|
|
|
| 18 |
Bu |
183 |
176 |
6.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12655.3 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 12174.4 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 B3LYP/3-21G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.502 |
0.571 |
0.000 |
| C2 |
-0.502 |
-0.571 |
0.000 |
| Br3 |
-0.502 |
2.275 |
0.000 |
| Br4 |
0.502 |
-2.275 |
0.000 |
| H5 |
1.120 |
0.566 |
0.896 |
| H6 |
1.120 |
0.566 |
-0.896 |
| H7 |
-1.120 |
-0.566 |
0.896 |
| H8 |
-1.120 |
-0.566 |
-0.896 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5196 | 1.9779 | 2.8459 | 1.0886 | 1.0886 | 2.1739 | 2.1739 |
C2 | 1.5196 | | 2.8459 | 1.9779 | 2.1739 | 2.1739 | 1.0886 | 1.0886 | Br3 | 1.9779 | 2.8459 | | 4.6598 | 2.5205 | 2.5205 | 3.0430 | 3.0430 | Br4 | 2.8459 | 1.9779 | 4.6598 | | 3.0430 | 3.0430 | 2.5205 | 2.5205 | H5 | 1.0886 | 2.1739 | 2.5205 | 3.0430 | | 1.7913 | 2.5106 | 3.0842 | H6 | 1.0886 | 2.1739 | 2.5205 | 3.0430 | 1.7913 | | 3.0842 | 2.5106 | H7 | 2.1739 | 1.0886 | 3.0430 | 2.5205 | 2.5106 | 3.0842 | | 1.7913 | H8 | 2.1739 | 1.0886 | 3.0430 | 2.5205 | 3.0842 | 2.5106 | 1.7913 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.201 |
|
C1 |
C2 |
H7 |
111.854 |
| C1 |
C2 |
H8 |
111.854 |
|
C2 |
C1 |
Br3 |
108.201 |
| C2 |
C1 |
H5 |
111.854 |
|
C2 |
C1 |
H6 |
111.854 |
| Br3 |
C1 |
H5 |
106.958 |
|
Br3 |
C1 |
H6 |
106.958 |
| Br4 |
C2 |
H7 |
106.958 |
|
Br4 |
C2 |
H8 |
106.958 |
| H5 |
C1 |
H6 |
110.734 |
|
H7 |
C2 |
H8 |
110.734 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.436 |
|
|
|
| 2 |
C |
-0.436 |
|
|
|
| 3 |
Br |
-0.070 |
|
|
|
| 4 |
Br |
-0.070 |
|
|
|
| 5 |
H |
0.253 |
|
|
|
| 6 |
H |
0.253 |
|
|
|
| 7 |
H |
0.253 |
|
|
|
| 8 |
H |
0.253 |
|
|
|
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 |
-47.823 |
0.910 |
0.000 |
| y |
0.910 |
-54.071 |
0.000 |
| z |
0.000 |
0.000 |
-48.706 |
|
| Traceless |
| | x | y | z |
| x |
3.565 |
0.910 |
0.000 |
| y |
0.910 |
-5.806 |
0.000 |
| z |
0.000 |
0.000 |
2.241 |
|
| Polar |
| 3z2-r2 | 4.482 |
| x2-y2 | 6.248 |
| xy | 0.910 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.183 |
-1.987 |
0.000 |
| y |
-1.987 |
11.588 |
0.000 |
| z |
0.000 |
0.000 |
5.215 |
<r2> (average value of r
2) Å
2
| <r2> |
427.780 |
| (<r2>)1/2 |
20.683 |
Jump to
S1C1
Energy calculated at B3LYP/3-21G*
| | hartrees |
| Energy at 0K | -5202.278162 |
| Energy at 298.15K | |
| HF Energy | -5202.278162 |
| Nuclear repulsion energy | 454.581155 |
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/3-21G*
| 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 |
3165 |
3045 |
0.05 |
95.09 |
0.75 |
0.86 |
| 2 |
A |
3106 |
2988 |
14.63 |
193.95 |
0.02 |
0.04 |
| 3 |
A |
1518 |
1461 |
0.25 |
8.17 |
0.68 |
0.81 |
| 4 |
A |
1342 |
1291 |
19.50 |
4.96 |
0.68 |
0.81 |
| 5 |
A |
1209 |
1163 |
2.64 |
21.04 |
0.75 |
0.86 |
| 6 |
A |
1011 |
973 |
1.44 |
3.12 |
0.74 |
0.85 |
| 7 |
A |
923 |
888 |
9.79 |
8.37 |
0.52 |
0.68 |
| 8 |
A |
572 |
550 |
7.86 |
17.43 |
0.09 |
0.17 |
| 9 |
A |
223 |
215 |
1.01 |
0.95 |
0.33 |
0.50 |
| 10 |
A |
79 |
76 |
0.15 |
0.91 |
0.73 |
0.84 |
| 11 |
B |
3182 |
3061 |
2.18 |
27.48 |
0.75 |
0.86 |
| 12 |
B |
3097 |
2979 |
1.74 |
59.14 |
0.75 |
0.86 |
| 13 |
B |
1521 |
1464 |
14.93 |
21.95 |
0.75 |
0.86 |
| 14 |
B |
1323 |
1273 |
45.31 |
0.60 |
0.75 |
0.86 |
| 15 |
B |
1162 |
1118 |
2.50 |
7.45 |
0.75 |
0.86 |
| 16 |
B |
856 |
824 |
20.29 |
0.83 |
0.75 |
0.86 |
| 17 |
B |
607 |
584 |
9.79 |
10.06 |
0.75 |
0.86 |
| 18 |
B |
357 |
344 |
6.18 |
3.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12626.3 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 12146.5 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/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.307 |
0.696 |
1.232 |
| C2 |
-0.307 |
-0.696 |
1.232 |
| Br3 |
-0.307 |
1.755 |
-0.305 |
| Br4 |
0.307 |
-1.755 |
-0.305 |
| H5 |
-0.001 |
1.244 |
2.126 |
| H6 |
1.394 |
0.653 |
1.172 |
| H7 |
0.001 |
-1.244 |
2.126 |
| H8 |
-1.394 |
-0.653 |
1.172 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5223 | 1.9655 | 2.8938 | 1.0925 | 1.0893 | 2.1580 | 2.1721 |
C2 | 1.5223 | | 2.8938 | 1.9655 | 2.1580 | 2.1721 | 1.0925 | 1.0893 | Br3 | 1.9655 | 2.8938 | | 3.5634 | 2.5033 | 2.5085 | 3.8730 | 3.0267 | Br4 | 2.8938 | 1.9655 | 3.5634 | | 3.8730 | 3.0267 | 2.5033 | 2.5085 | H5 | 1.0925 | 2.1580 | 2.5033 | 3.8730 | | 1.7907 | 2.4878 | 2.5390 | H6 | 1.0893 | 2.1721 | 2.5085 | 3.0267 | 1.7907 | | 2.5390 | 3.0785 | H7 | 2.1580 | 1.0925 | 3.8730 | 2.5033 | 2.4878 | 2.5390 | | 1.7907 | H8 | 2.1721 | 1.0893 | 3.0267 | 2.5085 | 2.5390 | 3.0785 | 1.7907 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
111.503 |
|
C1 |
C2 |
H7 |
110.147 |
| C1 |
C2 |
H8 |
111.472 |
|
C2 |
C1 |
Br3 |
111.503 |
| C2 |
C1 |
H5 |
110.147 |
|
C2 |
C1 |
H6 |
111.472 |
| Br3 |
C1 |
H5 |
106.363 |
|
Br3 |
C1 |
H6 |
106.871 |
| Br4 |
C2 |
H7 |
106.363 |
|
Br4 |
C2 |
H8 |
106.871 |
| H5 |
C1 |
H6 |
110.319 |
|
H7 |
C2 |
H8 |
110.319 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.440 |
|
|
|
| 2 |
C |
-0.440 |
|
|
|
| 3 |
Br |
-0.055 |
|
|
|
| 4 |
Br |
-0.055 |
|
|
|
| 5 |
H |
0.243 |
|
|
|
| 6 |
H |
0.252 |
|
|
|
| 7 |
H |
0.243 |
|
|
|
| 8 |
H |
0.252 |
|
|
|
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 |
2.469 |
2.469 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.384 |
0.683 |
0.000 |
| y |
0.683 |
-52.179 |
0.000 |
| z |
0.000 |
0.000 |
-43.962 |
|
| Traceless |
| | x | y | z |
| x |
-0.314 |
0.683 |
0.000 |
| y |
0.683 |
-6.006 |
0.000 |
| z |
0.000 |
0.000 |
6.320 |
|
| Polar |
| 3z2-r2 | 12.639 |
| x2-y2 | 3.795 |
| xy | 0.683 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.539 |
-0.764 |
0.000 |
| y |
-0.764 |
8.285 |
0.000 |
| z |
0.000 |
0.000 |
7.674 |
<r2> (average value of r
2) Å
2
| <r2> |
303.628 |
| (<r2>)1/2 |
17.425 |