Jump to
S1C2
Energy calculated at PBEPBE/6-31G*
| | hartrees |
| Energy at 0K | -958.580089 |
| Energy at 298.15K | |
| HF Energy | -958.580089 |
| Nuclear repulsion energy | 124.841325 |
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/6-31G*
| 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 |
3220 |
3174 |
0.01 |
|
|
|
| 2 |
A1 |
744 |
734 |
8.83 |
|
|
|
| 3 |
A1 |
309 |
304 |
0.27 |
|
|
|
| 4 |
B1 |
336i |
331i |
62.61 |
|
|
|
| 5 |
B2 |
1226 |
1208 |
47.91 |
|
|
|
| 6 |
B2 |
906 |
893 |
166.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3034.3 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 2990.9 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/6-31G*
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 |
1.757 |
| Cl3 |
0.000 |
1.489 |
-0.170 |
| Cl4 |
0.000 |
-1.489 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0879 | 1.7089 | 1.7089 |
H2 | 1.0879 | | 2.4351 | 2.4351 | Cl3 | 1.7089 | 2.4351 | | 2.9774 | Cl4 | 1.7089 | 2.4351 | 2.9774 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.412 |
|
Cl3 |
C1 |
Cl4 |
121.176 |
| Cl4 |
C1 |
H2 |
119.412 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.396 |
|
|
|
| 2 |
H |
0.240 |
|
|
|
| 3 |
Cl |
0.078 |
|
|
|
| 4 |
Cl |
0.078 |
|
|
|
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 |
0.923 |
0.923 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.700 |
0.000 |
0.000 |
| y |
0.000 |
-30.660 |
0.000 |
| z |
0.000 |
0.000 |
-28.694 |
|
| Traceless |
| | x | y | z |
| x |
-2.024 |
0.000 |
0.000 |
| y |
0.000 |
-0.462 |
0.000 |
| z |
0.000 |
0.000 |
2.486 |
|
| Polar |
| 3z2-r2 | 4.972 |
| x2-y2 | -1.041 |
| 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 |
2.274 |
0.000 |
0.000 |
| y |
0.000 |
6.848 |
0.000 |
| z |
0.000 |
0.000 |
3.712 |
<r2> (average value of r
2) Å
2
| <r2> |
101.064 |
| (<r2>)1/2 |
10.053 |
Jump to
S1C1
Energy calculated at PBEPBE/6-31G*
| | hartrees |
| Energy at 0K | -958.580759 |
| Energy at 298.15K | -958.581493 |
| HF Energy | -958.580759 |
| Nuclear repulsion energy | 124.643542 |
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/6-31G*
| 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' |
3178 |
3132 |
2.03 |
|
|
|
| 2 |
A' |
750 |
739 |
14.73 |
|
|
|
| 3 |
A' |
446 |
439 |
33.89 |
|
|
|
| 4 |
A' |
301 |
297 |
0.95 |
|
|
|
| 5 |
A" |
1230 |
1213 |
39.61 |
|
|
|
| 6 |
A" |
873 |
860 |
190.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3388.7 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 3340.3 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/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.693 |
0.000 |
| H2 |
-0.479 |
1.668 |
0.000 |
| Cl3 |
0.012 |
-0.171 |
1.486 |
| Cl4 |
0.012 |
-0.171 |
-1.486 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0911 | 1.7188 | 1.7188 |
H2 | 1.0911 | | 2.4145 | 2.4145 | Cl3 | 1.7188 | 2.4145 | | 2.9710 | Cl4 | 1.7188 | 2.4145 | 2.9710 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.694 |
|
Cl3 |
C1 |
Cl4 |
119.603 |
| Cl4 |
C1 |
H2 |
116.694 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.377 |
|
|
|
| 2 |
H |
0.237 |
|
|
|
| 3 |
Cl |
0.070 |
|
|
|
| 4 |
Cl |
0.070 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.541 |
0.825 |
0.000 |
0.986 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.422 |
-0.922 |
0.000 |
| y |
-0.922 |
-29.155 |
0.000 |
| z |
0.000 |
0.000 |
-30.817 |
|
| Traceless |
| | x | y | z |
| x |
-1.436 |
-0.922 |
0.000 |
| y |
-0.922 |
1.965 |
0.000 |
| z |
0.000 |
0.000 |
-0.529 |
|
| Polar |
| 3z2-r2 | -1.058 |
| x2-y2 | -2.267 |
| xy | -0.922 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.374 |
-0.203 |
0.000 |
| y |
-0.203 |
3.720 |
0.000 |
| z |
0.000 |
0.000 |
6.937 |
<r2> (average value of r
2) Å
2
| <r2> |
100.955 |
| (<r2>)1/2 |
10.048 |