Jump to
S1C2
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -958.645184 |
| Energy at 298.15K | |
| HF Energy | -958.645184 |
| Nuclear repulsion energy | 124.947766 |
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 PBEPBE/6-311G*
| 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 |
3194 |
3161 |
0.39 |
|
|
|
| 2 |
A1 |
737 |
729 |
7.13 |
|
|
|
| 3 |
A1 |
309 |
306 |
0.08 |
|
|
|
| 4 |
B1 |
348i |
344i |
65.69 |
|
|
|
| 5 |
B2 |
1219 |
1207 |
41.83 |
|
|
|
| 6 |
B2 |
892 |
882 |
182.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3001.5 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 2970.3 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 PBEPBE/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.669 |
| H2 |
0.000 |
0.000 |
1.755 |
| Cl3 |
0.000 |
1.487 |
-0.170 |
| Cl4 |
0.000 |
-1.487 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0852 | 1.7077 | 1.7077 |
H2 | 1.0852 | | 2.4321 | 2.4321 | Cl3 | 1.7077 | 2.4321 | | 2.9748 | Cl4 | 1.7077 | 2.4321 | 2.9748 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.427 |
|
Cl3 |
C1 |
Cl4 |
121.146 |
| Cl4 |
C1 |
H2 |
119.427 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.418 |
|
|
|
| 2 |
H |
0.304 |
|
|
|
| 3 |
Cl |
0.057 |
|
|
|
| 4 |
Cl |
0.057 |
|
|
|
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 |
0.897 |
0.897 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.555 |
0.000 |
0.000 |
| y |
0.000 |
-31.358 |
0.000 |
| z |
0.000 |
0.000 |
-29.407 |
|
| Traceless |
| | x | y | z |
| x |
-2.172 |
0.000 |
0.000 |
| y |
0.000 |
-0.378 |
0.000 |
| z |
0.000 |
0.000 |
2.550 |
|
| Polar |
| 3z2-r2 | 5.100 |
| x2-y2 | -1.196 |
| 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 |
2.239 |
0.000 |
0.000 |
| y |
0.000 |
7.342 |
0.000 |
| z |
0.000 |
0.000 |
3.744 |
<r2> (average value of r
2) Å
2
| <r2> |
101.393 |
| (<r2>)1/2 |
10.069 |
Jump to
S1C1
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -958.645951 |
| Energy at 298.15K | -958.646698 |
| HF Energy | -958.645951 |
| Nuclear repulsion energy | 124.726398 |
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 PBEPBE/6-311G*
| 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 |
3119 |
3.35 |
|
|
|
| 2 |
A' |
744 |
736 |
13.33 |
|
|
|
| 3 |
A' |
456 |
451 |
35.63 |
|
|
|
| 4 |
A' |
303 |
300 |
0.80 |
|
|
|
| 5 |
A" |
1228 |
1215 |
34.05 |
|
|
|
| 6 |
A" |
856 |
847 |
209.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3369.1 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 3334.0 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 PBEPBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.694 |
0.000 |
| H2 |
-0.493 |
1.658 |
0.000 |
| Cl3 |
0.012 |
-0.171 |
1.484 |
| Cl4 |
0.012 |
-0.171 |
-1.484 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0887 | 1.7182 | 1.7182 |
H2 | 1.0887 | | 2.4096 | 2.4096 | Cl3 | 1.7182 | 2.4096 | | 2.9688 | Cl4 | 1.7182 | 2.4096 | 2.9688 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.493 |
|
Cl3 |
C1 |
Cl4 |
119.521 |
| Cl4 |
C1 |
H2 |
116.493 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.399 |
|
|
|
| 2 |
H |
0.298 |
|
|
|
| 3 |
Cl |
0.051 |
|
|
|
| 4 |
Cl |
0.051 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.568 |
0.792 |
0.000 |
0.975 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.234 |
-0.980 |
0.000 |
| y |
-0.980 |
-29.907 |
0.000 |
| z |
0.000 |
0.000 |
-31.545 |
|
| Traceless |
| | x | y | z |
| x |
-1.508 |
-0.980 |
0.000 |
| y |
-0.980 |
1.982 |
0.000 |
| z |
0.000 |
0.000 |
-0.475 |
|
| Polar |
| 3z2-r2 | -0.950 |
| x2-y2 | -2.327 |
| xy | -0.980 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.336 |
-0.167 |
0.000 |
| y |
-0.167 |
3.781 |
0.000 |
| z |
0.000 |
0.000 |
7.439 |
<r2> (average value of r
2) Å
2
| <r2> |
101.307 |
| (<r2>)1/2 |
10.065 |