Jump to
S1C2
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -999.019008 |
| Energy at 298.15K | -999.023653 |
| Nuclear repulsion energy | 192.884926 |
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/6-31G*
Geometric Data calculated at B3LYP/6-31G*
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -999.016302 |
| Energy at 298.15K | -999.021086 |
| HF Energy | -999.016302 |
| Nuclear repulsion energy | 200.074226 |
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/6-31G*
| 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 |
3161 |
3035 |
0.66 |
|
|
|
| 2 |
A |
3104 |
2981 |
23.02 |
|
|
|
| 3 |
A |
1499 |
1440 |
0.17 |
|
|
|
| 4 |
A |
1365 |
1311 |
25.45 |
|
|
|
| 5 |
A |
1247 |
1197 |
1.29 |
|
|
|
| 6 |
A |
1055 |
1013 |
0.64 |
|
|
|
| 7 |
A |
962 |
923 |
13.51 |
|
|
|
| 8 |
A |
656 |
630 |
21.84 |
|
|
|
| 9 |
A |
260 |
250 |
1.00 |
|
|
|
| 10 |
A |
114 |
109 |
1.04 |
|
|
|
| 11 |
B |
3174 |
3048 |
6.61 |
|
|
|
| 12 |
B |
3095 |
2972 |
3.07 |
|
|
|
| 13 |
B |
1495 |
1436 |
10.59 |
|
|
|
| 14 |
B |
1343 |
1289 |
49.34 |
|
|
|
| 15 |
B |
1180 |
1133 |
1.14 |
|
|
|
| 16 |
B |
905 |
869 |
19.85 |
|
|
|
| 17 |
B |
681 |
654 |
30.62 |
|
|
|
| 18 |
B |
410 |
393 |
9.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12851.5 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 12341.3 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/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.297 |
0.697 |
0.895 |
| C2 |
-0.297 |
-0.697 |
0.895 |
| Cl3 |
-0.297 |
1.720 |
-0.471 |
| Cl4 |
0.297 |
-1.720 |
-0.471 |
| H5 |
0.009 |
1.208 |
1.818 |
| H6 |
1.386 |
0.666 |
0.826 |
| H7 |
-0.009 |
-1.208 |
1.818 |
| H8 |
-1.386 |
-0.666 |
0.826 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5164 | 1.8073 | 2.7767 | 1.0936 | 1.0910 | 2.1390 | 2.1675 |
C2 | 1.5164 | | 2.7767 | 1.8073 | 2.1390 | 2.1675 | 1.0936 | 1.0910 | Cl3 | 1.8073 | 2.7767 | | 3.4909 | 2.3659 | 2.3719 | 3.7277 | 2.9258 | Cl4 | 2.7767 | 1.8073 | 3.4909 | | 3.7277 | 2.9258 | 2.3659 | 2.3719 | H5 | 1.0936 | 2.1390 | 2.3659 | 3.7277 | | 1.7817 | 2.4156 | 2.5379 | H6 | 1.0910 | 2.1675 | 2.3719 | 2.9258 | 1.7817 | | 2.5379 | 3.0753 | H7 | 2.1390 | 1.0936 | 3.7277 | 2.3659 | 2.4156 | 2.5379 | | 1.7817 | H8 | 2.1675 | 1.0910 | 2.9258 | 2.3719 | 2.5379 | 3.0753 | 1.7817 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
113.031 |
|
C1 |
C2 |
H7 |
109.002 |
| C1 |
C2 |
H8 |
111.412 |
|
C2 |
C1 |
Cl3 |
113.031 |
| C2 |
C1 |
H5 |
109.002 |
|
C2 |
C1 |
H6 |
111.412 |
| Cl3 |
C1 |
H5 |
106.689 |
|
Cl3 |
C1 |
H6 |
107.253 |
| Cl4 |
C2 |
H7 |
106.689 |
|
Cl4 |
C2 |
H8 |
107.253 |
| H5 |
C1 |
H6 |
109.294 |
|
H7 |
C2 |
H8 |
109.294 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.355 |
|
|
|
| 2 |
C |
-0.355 |
|
|
|
| 3 |
Cl |
-0.064 |
|
|
|
| 4 |
Cl |
-0.064 |
|
|
|
| 5 |
H |
0.203 |
|
|
|
| 6 |
H |
0.216 |
|
|
|
| 7 |
H |
0.203 |
|
|
|
| 8 |
H |
0.216 |
|
|
|
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 |
2.931 |
2.931 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.300 |
1.272 |
0.000 |
| y |
1.272 |
-42.386 |
0.000 |
| z |
0.000 |
0.000 |
-35.189 |
|
| Traceless |
| | x | y | z |
| x |
1.487 |
1.272 |
0.000 |
| y |
1.272 |
-6.142 |
0.000 |
| z |
0.000 |
0.000 |
4.655 |
|
| Polar |
| 3z2-r2 | 9.309 |
| x2-y2 | 5.086 |
| xy | 1.272 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.682 |
-0.620 |
0.000 |
| y |
-0.620 |
6.768 |
0.000 |
| z |
0.000 |
0.000 |
6.315 |
<r2> (average value of r
2) Å
2
| <r2> |
167.185 |
| (<r2>)1/2 |
12.930 |