Jump to
S1C2
Vibrational Frequencies calculated at B3LYP/6-311+G(3df,2p)
Geometric Data calculated at B3LYP/6-311+G(3df,2p)
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B3LYP/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -3113.032715 |
| Energy at 298.15K | |
| HF Energy | -3113.032715 |
| Nuclear repulsion energy | 302.497508 |
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/6-311+G(3df,2p)
| 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 |
3152 |
3048 |
0.77 |
36.57 |
0.75 |
0.86 |
| 2 |
A |
3127 |
3024 |
0.89 |
69.48 |
0.75 |
0.86 |
| 3 |
A |
3084 |
2983 |
10.50 |
164.22 |
0.03 |
0.07 |
| 4 |
A |
3061 |
2960 |
8.36 |
112.75 |
0.17 |
0.29 |
| 5 |
A |
1473 |
1424 |
5.79 |
5.44 |
0.75 |
0.86 |
| 6 |
A |
1467 |
1419 |
7.84 |
6.05 |
0.73 |
0.84 |
| 7 |
A |
1328 |
1284 |
18.84 |
1.70 |
0.33 |
0.49 |
| 8 |
A |
1290 |
1247 |
50.33 |
4.89 |
0.31 |
0.48 |
| 9 |
A |
1205 |
1166 |
1.89 |
5.37 |
0.72 |
0.84 |
| 10 |
A |
1142 |
1105 |
0.69 |
1.30 |
0.67 |
0.80 |
| 11 |
A |
1035 |
1000 |
2.19 |
1.09 |
0.73 |
0.84 |
| 12 |
A |
928 |
897 |
8.93 |
4.25 |
0.18 |
0.31 |
| 13 |
A |
869 |
841 |
19.64 |
1.08 |
0.75 |
0.85 |
| 14 |
A |
664 |
642 |
22.48 |
9.24 |
0.29 |
0.45 |
| 15 |
A |
562 |
544 |
12.13 |
18.97 |
0.13 |
0.23 |
| 16 |
A |
383 |
371 |
7.76 |
1.92 |
0.67 |
0.80 |
| 17 |
A |
240 |
232 |
1.39 |
1.48 |
0.19 |
0.32 |
| 18 |
A |
95 |
92 |
0.54 |
0.97 |
0.65 |
0.79 |
Unscaled Zero Point Vibrational Energy (zpe) 12552.5 cm
-1
Scaled (by 0.967) Zero Point Vibrational Energy (zpe) 12138.3 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 B3LYP/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.020 |
1.099 |
-0.385 |
| C2 |
1.290 |
0.896 |
0.404 |
| Br3 |
-1.373 |
-0.224 |
0.035 |
| Cl4 |
2.198 |
-0.575 |
-0.086 |
| H5 |
-0.414 |
2.065 |
-0.141 |
| H6 |
0.189 |
1.030 |
-1.454 |
| H7 |
1.955 |
1.741 |
0.228 |
| H8 |
1.094 |
0.810 |
1.469 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5086 | 1.9663 | 2.7628 | 1.0872 | 1.0849 | 2.1292 | 2.1621 |
C2 | 1.5086 | | 2.9120 | 1.7971 | 2.1368 | 2.1642 | 1.0894 | 1.0860 | Br3 | 1.9663 | 2.9120 | | 3.5899 | 2.4880 | 2.4962 | 3.8695 | 3.0349 | Cl4 | 2.7628 | 1.7971 | 3.5899 | | 3.7141 | 2.9125 | 2.3490 | 2.3569 | H5 | 1.0872 | 2.1368 | 2.4880 | 3.7141 | | 1.7779 | 2.4200 | 2.5380 | H6 | 1.0849 | 2.1642 | 2.4962 | 2.9125 | 1.7779 | | 2.5409 | 3.0683 | H7 | 2.1292 | 1.0894 | 3.8695 | 2.3490 | 2.4200 | 2.5409 | | 1.7739 | H8 | 2.1621 | 1.0860 | 3.0349 | 2.3569 | 2.5380 | 3.0683 | 1.7739 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
113.104 |
|
C1 |
C2 |
H7 |
109.020 |
| C1 |
C2 |
H8 |
111.845 |
|
C2 |
C1 |
Br3 |
113.204 |
| C2 |
C1 |
Cl4 |
36.749 |
|
C2 |
C1 |
H6 |
112.093 |
| Br3 |
C1 |
H5 |
105.490 |
|
Br3 |
C1 |
H6 |
106.166 |
| Cl4 |
C2 |
H7 |
106.338 |
|
Cl4 |
C2 |
H8 |
107.071 |
| H5 |
C1 |
H6 |
109.877 |
|
H7 |
C2 |
H8 |
109.264 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.142 |
|
|
|
| 2 |
C |
-0.268 |
|
|
|
| 3 |
Br |
-0.109 |
|
|
|
| 4 |
Cl |
-0.246 |
|
|
|
| 5 |
H |
0.184 |
|
|
|
| 6 |
H |
0.191 |
|
|
|
| 7 |
H |
0.191 |
|
|
|
| 8 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.387 |
2.649 |
0.097 |
2.678 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.317 |
2.654 |
0.496 |
| y |
2.654 |
-40.981 |
-0.090 |
| z |
0.496 |
-0.090 |
-43.643 |
|
| Traceless |
| | x | y | z |
| x |
-6.005 |
2.654 |
0.496 |
| y |
2.654 |
4.998 |
-0.090 |
| z |
0.496 |
-0.090 |
1.006 |
|
| Polar |
| 3z2-r2 | 2.013 |
| x2-y2 | -7.335 |
| xy | 2.654 |
| xz | 0.496 |
| yz | -0.090 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.794 |
0.188 |
-0.172 |
| y |
0.188 |
9.094 |
0.032 |
| z |
-0.172 |
0.032 |
7.663 |
<r2> (average value of r
2) Å
2
| <r2> |
225.799 |
| (<r2>)1/2 |
15.027 |