Jump to
S1C2
Energy calculated at HSEh1PBE/3-21G
| | hartrees |
| Energy at 0K | -954.063328 |
| Energy at 298.15K | |
| HF Energy | -954.063328 |
| Nuclear repulsion energy | 121.370419 |
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 HSEh1PBE/3-21G
| 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 |
3335 |
3212 |
2.72 |
|
|
|
| 2 |
A1 |
673 |
648 |
15.72 |
|
|
|
| 3 |
A1 |
282 |
271 |
0.73 |
|
|
|
| 4 |
B1 |
413i |
398i |
105.06 |
|
|
|
| 5 |
B2 |
1189 |
1146 |
57.21 |
|
|
|
| 6 |
B2 |
828 |
798 |
157.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2946.7 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 2838.6 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 HSEh1PBE/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.722 |
| H2 |
0.000 |
0.000 |
1.797 |
| Cl3 |
0.000 |
1.523 |
-0.180 |
| Cl4 |
0.000 |
-1.523 |
-0.180 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0758 | 1.7698 | 1.7698 |
H2 | 1.0758 | | 2.4960 | 2.4960 | Cl3 | 1.7698 | 2.4960 | | 3.0456 | Cl4 | 1.7698 | 2.4960 | 3.0456 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
120.636 |
|
Cl3 |
C1 |
Cl4 |
118.728 |
| Cl4 |
C1 |
H2 |
120.636 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.632 |
|
|
|
| 2 |
H |
0.318 |
|
|
|
| 3 |
Cl |
0.157 |
|
|
|
| 4 |
Cl |
0.157 |
|
|
|
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 |
1.316 |
1.316 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.527 |
0.000 |
0.000 |
| y |
0.000 |
-32.528 |
0.000 |
| z |
0.000 |
0.000 |
-28.896 |
|
| Traceless |
| | x | y | z |
| x |
-1.815 |
0.000 |
0.000 |
| y |
0.000 |
-1.816 |
0.000 |
| z |
0.000 |
0.000 |
3.631 |
|
| Polar |
| 3z2-r2 | 7.263 |
| x2-y2 | 0.001 |
| 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 |
1.385 |
0.000 |
0.000 |
| y |
0.000 |
6.483 |
0.000 |
| z |
0.000 |
0.000 |
3.091 |
<r2> (average value of r
2) Å
2
| <r2> |
105.862 |
| (<r2>)1/2 |
10.289 |
Jump to
S1C1
Energy calculated at HSEh1PBE/3-21G
| | hartrees |
| Energy at 0K | -954.064872 |
| Energy at 298.15K | -954.065593 |
| HF Energy | -954.064872 |
| Nuclear repulsion energy | 120.804501 |
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 HSEh1PBE/3-21G
| 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' |
3268 |
3148 |
2.10 |
|
|
|
| 2 |
A' |
702 |
676 |
33.46 |
|
|
|
| 3 |
A' |
510 |
491 |
24.08 |
|
|
|
| 4 |
A' |
280 |
269 |
0.62 |
|
|
|
| 5 |
A" |
1217 |
1173 |
38.22 |
|
|
|
| 6 |
A" |
782 |
753 |
188.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3379.0 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 3254.9 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 HSEh1PBE/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.015 |
0.757 |
0.000 |
| H2 |
-0.581 |
1.660 |
0.000 |
| Cl3 |
0.015 |
-0.182 |
1.522 |
| Cl4 |
0.015 |
-0.182 |
-1.522 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0815 | 1.7891 | 1.7891 |
H2 | 1.0815 | | 2.4632 | 2.4632 | Cl3 | 1.7891 | 2.4632 | | 3.0448 | Cl4 | 1.7891 | 2.4632 | 3.0448 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.006 |
|
Cl3 |
C1 |
Cl4 |
116.623 |
| Cl4 |
C1 |
H2 |
116.006 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.578 |
|
|
|
| 2 |
H |
0.315 |
|
|
|
| 3 |
Cl |
0.132 |
|
|
|
| 4 |
Cl |
0.132 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.812 |
1.186 |
0.000 |
1.437 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.060 |
-1.271 |
0.000 |
| y |
-1.271 |
-29.685 |
0.000 |
| z |
0.000 |
0.000 |
-32.922 |
|
| Traceless |
| | x | y | z |
| x |
-0.756 |
-1.271 |
0.000 |
| y |
-1.271 |
2.806 |
0.000 |
| z |
0.000 |
0.000 |
-2.049 |
|
| Polar |
| 3z2-r2 | -4.098 |
| x2-y2 | -2.375 |
| xy | -1.271 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.537 |
-0.245 |
0.000 |
| y |
-0.245 |
3.139 |
0.000 |
| z |
0.000 |
0.000 |
6.655 |
<r2> (average value of r
2) Å
2
| <r2> |
106.188 |
| (<r2>)1/2 |
10.305 |