Vibrational Frequencies calculated at B3PW91/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3099 |
2965 |
23.49 |
|
|
|
| 2 |
A1 |
1417 |
1355 |
14.59 |
|
|
|
| 3 |
A1 |
747 |
715 |
27.37 |
|
|
|
| 4 |
E |
3204 |
3065 |
6.34 |
|
|
|
| 4 |
E |
3204 |
3065 |
6.34 |
|
|
|
| 5 |
E |
1507 |
1441 |
7.21 |
|
|
|
| 5 |
E |
1507 |
1441 |
7.21 |
|
|
|
| 6 |
E |
1051 |
1005 |
5.09 |
|
|
|
| 6 |
E |
1051 |
1005 |
5.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8392.4 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 8029.0 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.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.593 |
|
|
|
| 2 |
Cl |
-0.076 |
|
|
|
| 3 |
H |
0.223 |
|
|
|
| 4 |
H |
0.223 |
|
|
|
| 5 |
H |
0.223 |
|
|
|
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 |
-2.068 |
2.068 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.005 |
0.000 |
2.112 |
2.112 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.675 |
0.000 |
0.000 |
| y |
0.000 |
-19.675 |
0.000 |
| z |
0.000 |
0.000 |
-17.889 |
|
| Traceless |
| | x | y | z |
| x |
-0.893 |
0.000 |
0.000 |
| y |
0.000 |
-0.893 |
0.000 |
| z |
0.000 |
0.000 |
1.786 |
|
| Polar |
| 3z2-r2 | 3.571 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.412 |
0.000 |
0.000 |
| y |
0.000 |
2.412 |
0.000 |
| z |
0.000 |
0.000 |
4.087 |
<r2> (average value of r
2) Å
2
| <r2> |
36.707 |
| (<r2>)1/2 |
6.059 |