Jump to
S1C2
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -5227.118036 |
| Energy at 298.15K | -5227.128155 |
| HF Energy | -5227.118036 |
| Nuclear repulsion energy | 414.285422 |
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/cc-pVTZ
| 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 |
3109 |
3005 |
0.00 |
|
|
|
| 2 |
Ag |
1492 |
1442 |
0.00 |
|
|
|
| 3 |
Ag |
1280 |
1237 |
0.00 |
|
|
|
| 4 |
Ag |
1062 |
1026 |
0.00 |
|
|
|
| 5 |
Ag |
649 |
627 |
0.00 |
|
|
|
| 6 |
Ag |
185 |
178 |
0.00 |
|
|
|
| 7 |
Au |
3189 |
3083 |
0.31 |
|
|
|
| 8 |
Au |
1101 |
1064 |
2.91 |
|
|
|
| 9 |
Au |
762 |
737 |
4.19 |
|
|
|
| 10 |
Au |
103 |
99 |
4.48 |
|
|
|
| 11 |
Bg |
3166 |
3060 |
0.00 |
|
|
|
| 12 |
Bg |
1288 |
1245 |
0.00 |
|
|
|
| 13 |
Bg |
943 |
912 |
0.00 |
|
|
|
| 14 |
Bu |
3118 |
3014 |
5.47 |
|
|
|
| 15 |
Bu |
1489 |
1439 |
7.27 |
|
|
|
| 16 |
Bu |
1211 |
1171 |
55.10 |
|
|
|
| 17 |
Bu |
573 |
554 |
77.27 |
|
|
|
| 18 |
Bu |
178 |
172 |
6.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12448.8 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 12033.0 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/cc-pVTZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.493 |
0.568 |
0.000 |
| C2 |
-0.493 |
-0.568 |
0.000 |
| Br3 |
-0.493 |
2.284 |
0.000 |
| Br4 |
0.493 |
-2.284 |
0.000 |
| H5 |
1.113 |
0.580 |
0.889 |
| H6 |
1.113 |
0.580 |
-0.889 |
| H7 |
-1.113 |
-0.580 |
0.889 |
| H8 |
-1.113 |
-0.580 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5041 | 1.9797 | 2.8517 | 1.0839 | 1.0839 | 2.1651 | 2.1651 |
C2 | 1.5041 | | 2.8517 | 1.9797 | 2.1651 | 2.1651 | 1.0839 | 1.0839 | Br3 | 1.9797 | 2.8517 | | 4.6735 | 2.5047 | 2.5047 | 3.0624 | 3.0624 | Br4 | 2.8517 | 1.9797 | 4.6735 | | 3.0624 | 3.0624 | 2.5047 | 2.5047 | H5 | 1.0839 | 2.1651 | 2.5047 | 3.0624 | | 1.7788 | 2.5097 | 3.0762 | H6 | 1.0839 | 2.1651 | 2.5047 | 3.0624 | 1.7788 | | 3.0762 | 2.5097 | H7 | 2.1651 | 1.0839 | 3.0624 | 2.5047 | 2.5097 | 3.0762 | | 1.7788 | H8 | 2.1651 | 1.0839 | 3.0624 | 2.5047 | 3.0762 | 2.5097 | 1.7788 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.120 |
|
C1 |
C2 |
H7 |
112.552 |
| C1 |
C2 |
H8 |
112.552 |
|
C2 |
C1 |
Br3 |
109.120 |
| C2 |
C1 |
H5 |
112.552 |
|
C2 |
C1 |
H6 |
112.552 |
| Br3 |
C1 |
H5 |
105.951 |
|
Br3 |
C1 |
H6 |
105.951 |
| Br4 |
C2 |
H7 |
105.951 |
|
Br4 |
C2 |
H8 |
105.951 |
| H5 |
C1 |
H6 |
110.278 |
|
H7 |
C2 |
H8 |
110.278 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.160 |
|
|
|
| 2 |
C |
-0.160 |
|
|
|
| 3 |
Br |
-0.125 |
|
|
|
| 4 |
Br |
-0.125 |
|
|
|
| 5 |
H |
0.143 |
|
|
|
| 6 |
H |
0.143 |
|
|
|
| 7 |
H |
0.143 |
|
|
|
| 8 |
H |
0.143 |
|
|
|
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 |
-49.183 |
1.433 |
0.000 |
| y |
1.433 |
-56.333 |
0.000 |
| z |
0.000 |
0.000 |
-49.751 |
|
| Traceless |
| | x | y | z |
| x |
3.859 |
1.433 |
0.000 |
| y |
1.433 |
-6.866 |
0.000 |
| z |
0.000 |
0.000 |
3.007 |
|
| Polar |
| 3z2-r2 | 6.013 |
| x2-y2 | 7.150 |
| xy | 1.433 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.801 |
-2.017 |
0.000 |
| y |
-2.017 |
14.147 |
0.000 |
| z |
0.000 |
0.000 |
6.630 |
<r2> (average value of r
2) Å
2
| <r2> |
430.800 |
| (<r2>)1/2 |
20.756 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -5227.114089 |
| Energy at 298.15K | |
| HF Energy | -5227.114089 |
| Nuclear repulsion energy | 446.886954 |
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/cc-pVTZ
| 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 |
3144 |
3039 |
0.00 |
90.87 |
0.74 |
0.85 |
| 2 |
A |
3087 |
2984 |
14.48 |
252.22 |
0.02 |
0.04 |
| 3 |
A |
1468 |
1419 |
0.64 |
3.29 |
0.73 |
0.84 |
| 4 |
A |
1307 |
1263 |
20.09 |
3.59 |
0.35 |
0.52 |
| 5 |
A |
1188 |
1148 |
1.69 |
9.04 |
0.75 |
0.86 |
| 6 |
A |
1031 |
996 |
1.36 |
1.88 |
0.58 |
0.73 |
| 7 |
A |
903 |
873 |
8.32 |
6.65 |
0.38 |
0.55 |
| 8 |
A |
545 |
527 |
8.19 |
19.89 |
0.06 |
0.11 |
| 9 |
A |
225 |
218 |
1.31 |
1.77 |
0.38 |
0.55 |
| 10 |
A |
76 |
73 |
0.25 |
1.27 |
0.70 |
0.82 |
| 11 |
B |
3158 |
3053 |
1.10 |
25.08 |
0.75 |
0.86 |
| 12 |
B |
3078 |
2975 |
1.96 |
51.25 |
0.75 |
0.86 |
| 13 |
B |
1465 |
1416 |
11.50 |
10.87 |
0.75 |
0.86 |
| 14 |
B |
1277 |
1235 |
71.20 |
4.00 |
0.75 |
0.86 |
| 15 |
B |
1122 |
1084 |
1.77 |
3.27 |
0.75 |
0.86 |
| 16 |
B |
847 |
819 |
19.39 |
1.18 |
0.75 |
0.86 |
| 17 |
B |
579 |
559 |
17.80 |
9.94 |
0.75 |
0.86 |
| 18 |
B |
352 |
340 |
6.82 |
2.54 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12425.1 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 12010.1 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 B3LYP/cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.313 |
0.685 |
1.178 |
| C2 |
-0.313 |
-0.685 |
1.178 |
| Br3 |
-0.313 |
1.831 |
-0.293 |
| Br4 |
0.313 |
-1.831 |
-0.293 |
| H5 |
0.036 |
1.212 |
2.089 |
| H6 |
1.393 |
0.646 |
1.092 |
| H7 |
-0.036 |
-1.212 |
2.089 |
| H8 |
-1.393 |
-0.646 |
1.092 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5066 | 1.9663 | 2.9149 | 1.0878 | 1.0847 | 2.1331 | 2.1653 |
C2 | 1.5066 | | 2.9149 | 1.9663 | 2.1331 | 2.1653 | 1.0878 | 1.0847 | Br3 | 1.9663 | 2.9149 | | 3.7158 | 2.4852 | 2.4966 | 3.8740 | 3.0369 | Br4 | 2.9149 | 1.9663 | 3.7158 | | 3.8740 | 3.0369 | 2.4852 | 2.4966 | H5 | 1.0878 | 2.1331 | 2.4852 | 3.8740 | | 1.7764 | 2.4243 | 2.5464 | H6 | 1.0847 | 2.1653 | 2.4966 | 3.0369 | 1.7764 | | 2.5464 | 3.0710 | H7 | 2.1331 | 1.0878 | 3.8740 | 2.4852 | 2.4243 | 2.5464 | | 1.7764 | H8 | 2.1653 | 1.0847 | 3.0369 | 2.4966 | 2.5464 | 3.0710 | 1.7764 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.480 |
|
C1 |
C2 |
H7 |
109.545 |
| C1 |
C2 |
H8 |
112.337 |
|
C2 |
C1 |
Br3 |
113.480 |
| C2 |
C1 |
H5 |
109.545 |
|
C2 |
C1 |
H6 |
112.337 |
| Br3 |
C1 |
H5 |
105.272 |
|
Br3 |
C1 |
H6 |
106.201 |
| Br4 |
C2 |
H7 |
105.272 |
|
Br4 |
C2 |
H8 |
106.201 |
| H5 |
C1 |
H6 |
109.708 |
|
H7 |
C2 |
H8 |
109.708 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.167 |
|
|
|
| 2 |
C |
-0.167 |
|
|
|
| 3 |
Br |
-0.107 |
|
|
|
| 4 |
Br |
-0.107 |
|
|
|
| 5 |
H |
0.136 |
|
|
|
| 6 |
H |
0.138 |
|
|
|
| 7 |
H |
0.136 |
|
|
|
| 8 |
H |
0.138 |
|
|
|
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 |
2.643 |
2.643 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.526 |
0.949 |
0.000 |
| y |
0.949 |
-54.248 |
0.000 |
| z |
0.000 |
0.000 |
-45.441 |
|
| Traceless |
| | x | y | z |
| x |
0.319 |
0.949 |
0.000 |
| y |
0.949 |
-6.765 |
0.000 |
| z |
0.000 |
0.000 |
6.446 |
|
| Polar |
| 3z2-r2 | 12.892 |
| x2-y2 | 4.722 |
| xy | 0.949 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.081 |
-0.795 |
0.000 |
| y |
-0.795 |
10.699 |
0.000 |
| z |
0.000 |
0.000 |
9.130 |
<r2> (average value of r
2) Å
2
| <r2> |
320.907 |
| (<r2>)1/2 |
17.914 |