Jump to
S1C2
Energy calculated at PBE1PBE/6-31G*
| hartrees |
Energy at 0K | -958.658469 |
Energy at 298.15K | |
HF Energy | -958.658469 |
Nuclear repulsion energy | 125.901970 |
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 PBE1PBE/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 |
3314 |
3149 |
0.16 |
|
|
|
2 |
A1 |
776 |
737 |
10.52 |
|
|
|
3 |
A1 |
320 |
304 |
0.42 |
|
|
|
4 |
B1 |
330i |
313i |
59.66 |
|
|
|
5 |
B2 |
1275 |
1211 |
55.56 |
|
|
|
6 |
B2 |
957 |
909 |
156.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3155.4 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 2998.6 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 PBE1PBE/6-31G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.667 |
H2 |
0.000 |
0.000 |
1.746 |
Cl3 |
0.000 |
1.475 |
-0.169 |
Cl4 |
0.000 |
-1.475 |
-0.169 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0799 | 1.6952 | 1.6952 |
H2 | 1.0799 | | 2.4175 | 2.4175 | Cl3 | 1.6952 | 2.4175 | | 2.9501 | Cl4 | 1.6952 | 2.4175 | 2.9501 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.529 |
|
Cl3 |
C1 |
Cl4 |
120.942 |
Cl4 |
C1 |
H2 |
119.529 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.404 |
|
|
|
2 |
H |
0.259 |
|
|
|
3 |
Cl |
0.073 |
|
|
|
4 |
Cl |
0.073 |
|
|
|
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 |
1.013 |
1.013 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.715 |
0.000 |
0.000 |
y |
0.000 |
-30.908 |
0.000 |
z |
0.000 |
0.000 |
-28.639 |
|
Traceless |
| x | y | z |
x |
-1.941 |
0.000 |
0.000 |
y |
0.000 |
-0.731 |
0.000 |
z |
0.000 |
0.000 |
2.672 |
|
Polar |
3z2-r2 | 5.344 |
x2-y2 | -0.807 |
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 |
2.248 |
0.000 |
0.000 |
y |
0.000 |
6.450 |
0.000 |
z |
0.000 |
0.000 |
3.620 |
<r2> (average value of r
2) Å
2
<r2> |
99.662 |
(<r2>)1/2 |
9.983 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-31G*
| hartrees |
Energy at 0K | -958.659001 |
Energy at 298.15K | -958.659778 |
HF Energy | -958.659001 |
Nuclear repulsion energy | 125.782780 |
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 PBE1PBE/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' |
3280 |
3117 |
1.51 |
|
|
|
2 |
A' |
781 |
742 |
15.28 |
|
|
|
3 |
A' |
446 |
424 |
33.99 |
|
|
|
4 |
A' |
312 |
296 |
1.46 |
|
|
|
5 |
A" |
1280 |
1217 |
47.78 |
|
|
|
6 |
A" |
931 |
885 |
177.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3515.1 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 3340.4 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 PBE1PBE/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.011 |
0.686 |
0.000 |
H2 |
-0.441 |
1.669 |
0.000 |
Cl3 |
0.011 |
-0.170 |
1.472 |
Cl4 |
0.011 |
-0.170 |
-1.472 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0824 | 1.7027 | 1.7027 |
H2 | 1.0824 | | 2.3989 | 2.3989 | Cl3 | 1.7027 | 2.3989 | | 2.9439 | Cl4 | 1.7027 | 2.3989 | 2.9439 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
117.181 |
|
Cl3 |
C1 |
Cl4 |
119.646 |
Cl4 |
C1 |
H2 |
117.181 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.385 |
|
|
|
2 |
H |
0.255 |
|
|
|
3 |
Cl |
0.065 |
|
|
|
4 |
Cl |
0.065 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.496 |
0.930 |
0.000 |
1.055 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.470 |
-0.863 |
0.000 |
y |
-0.863 |
-29.040 |
0.000 |
z |
0.000 |
0.000 |
-31.043 |
|
Traceless |
| x | y | z |
x |
-1.428 |
-0.863 |
0.000 |
y |
-0.863 |
2.216 |
0.000 |
z |
0.000 |
0.000 |
-0.788 |
|
Polar |
3z2-r2 | -1.576 |
x2-y2 | -2.430 |
xy | -0.863 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.331 |
-0.182 |
0.000 |
y |
-0.182 |
3.620 |
0.000 |
z |
0.000 |
0.000 |
6.509 |
<r2> (average value of r
2) Å
2
<r2> |
99.518 |
(<r2>)1/2 |
9.976 |