Jump to
S1C2
Energy calculated at PBE1PBE/6-31G
| | hartrees |
| Energy at 0K | -958.599109 |
| Energy at 298.15K | |
| HF Energy | -958.599109 |
| Nuclear repulsion energy | 121.942471 |
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 |
3355 |
3207 |
0.95 |
|
|
|
| 2 |
A1 |
710 |
678 |
14.46 |
|
|
|
| 3 |
A1 |
299 |
286 |
0.71 |
|
|
|
| 4 |
B1 |
350i |
335i |
94.88 |
|
|
|
| 5 |
B2 |
1241 |
1186 |
53.36 |
|
|
|
| 6 |
B2 |
887 |
848 |
159.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3070.8 cm
-1
Scaled (by 0.9559) Zero Point Vibrational Energy (zpe) 2935.4 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 C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.698 |
| H2 |
0.000 |
0.000 |
1.774 |
| Cl3 |
0.000 |
1.523 |
-0.175 |
| Cl4 |
0.000 |
-1.523 |
-0.175 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0764 | 1.7553 | 1.7553 |
H2 | 1.0764 | | 2.4737 | 2.4737 | Cl3 | 1.7553 | 2.4737 | | 3.0454 | Cl4 | 1.7553 | 2.4737 | 3.0454 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.831 |
|
Cl3 |
C1 |
Cl4 |
120.337 |
| Cl4 |
C1 |
H2 |
119.831 |
|
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 |
-0.532 |
|
|
|
| 2 |
H |
0.264 |
|
|
|
| 3 |
Cl |
0.134 |
|
|
|
| 4 |
Cl |
0.134 |
|
|
|
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 |
1.295 |
1.295 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.083 |
0.000 |
0.000 |
| y |
0.000 |
-32.364 |
0.000 |
| z |
0.000 |
0.000 |
-28.777 |
|
| Traceless |
| | x | y | z |
| x |
-1.512 |
0.000 |
0.000 |
| y |
0.000 |
-1.934 |
0.000 |
| z |
0.000 |
0.000 |
3.446 |
|
| Polar |
| 3z2-r2 | 6.892 |
| x2-y2 | 0.281 |
| 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 |
1.610 |
0.000 |
0.000 |
| y |
0.000 |
6.571 |
0.000 |
| z |
0.000 |
0.000 |
3.213 |
<r2> (average value of r
2) Å
2
| <r2> |
105.355 |
| (<r2>)1/2 |
10.264 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-31G
| | hartrees |
| Energy at 0K | -958.599846 |
| Energy at 298.15K | -958.600575 |
| HF Energy | -958.599846 |
| Nuclear repulsion energy | 121.680790 |
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' |
3309 |
3163 |
1.12 |
|
|
|
| 2 |
A' |
721 |
690 |
24.54 |
|
|
|
| 3 |
A' |
458 |
438 |
39.64 |
|
|
|
| 4 |
A' |
294 |
281 |
0.96 |
|
|
|
| 5 |
A" |
1253 |
1198 |
42.01 |
|
|
|
| 6 |
A" |
854 |
816 |
183.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3445.0 cm
-1
Scaled (by 0.9559) Zero Point Vibrational Energy (zpe) 3293.0 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 PBE1PBE/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.722 |
0.000 |
| H2 |
-0.480 |
1.683 |
0.000 |
| Cl3 |
0.012 |
-0.177 |
1.521 |
| Cl4 |
0.012 |
-0.177 |
-1.521 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0802 | 1.7663 | 1.7663 |
H2 | 1.0802 | | 2.4524 | 2.4524 | Cl3 | 1.7663 | 2.4524 | | 3.0412 | Cl4 | 1.7663 | 2.4524 | 3.0412 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.927 |
|
Cl3 |
C1 |
Cl4 |
118.841 |
| Cl4 |
C1 |
H2 |
116.927 |
|
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 |
-0.498 |
|
|
|
| 2 |
H |
0.260 |
|
|
|
| 3 |
Cl |
0.119 |
|
|
|
| 4 |
Cl |
0.119 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.667 |
1.206 |
0.000 |
1.378 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.778 |
-1.044 |
0.000 |
| y |
-1.044 |
-29.293 |
0.000 |
| z |
0.000 |
0.000 |
-32.611 |
|
| Traceless |
| | x | y | z |
| x |
-0.826 |
-1.044 |
0.000 |
| y |
-1.044 |
2.901 |
0.000 |
| z |
0.000 |
0.000 |
-2.076 |
|
| Polar |
| 3z2-r2 | -4.152 |
| x2-y2 | -2.485 |
| xy | -1.044 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.707 |
-0.202 |
0.000 |
| y |
-0.202 |
3.237 |
0.000 |
| z |
0.000 |
0.000 |
6.668 |
<r2> (average value of r
2) Å
2
| <r2> |
105.380 |
| (<r2>)1/2 |
10.265 |