Jump to
S1C2
Energy calculated at wB97X-D/6-31G
| | hartrees |
| Energy at 0K | -958.926864 |
| Energy at 298.15K | |
| HF Energy | -958.926864 |
| Nuclear repulsion energy | 121.810097 |
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 wB97X-D/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 |
3354 |
3354 |
0.95 |
|
|
|
| 2 |
A1 |
716 |
716 |
14.95 |
|
|
|
| 3 |
A1 |
299 |
299 |
0.87 |
|
|
|
| 4 |
B1 |
375i |
375i |
95.73 |
|
|
|
| 5 |
B2 |
1239 |
1239 |
57.42 |
|
|
|
| 6 |
B2 |
899 |
899 |
151.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3065.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3065.6 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 wB97X-D/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.701 |
| H2 |
0.000 |
0.000 |
1.777 |
| Cl3 |
0.000 |
1.524 |
-0.176 |
| Cl4 |
0.000 |
-1.524 |
-0.176 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0764 | 1.7578 | 1.7578 |
H2 | 1.0764 | | 2.4770 | 2.4770 | Cl3 | 1.7578 | 2.4770 | | 3.0474 | Cl4 | 1.7578 | 2.4770 | 3.0474 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.908 |
|
Cl3 |
C1 |
Cl4 |
120.183 |
| Cl4 |
C1 |
H2 |
119.908 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.511 |
|
|
|
| 2 |
H |
0.262 |
|
|
|
| 3 |
Cl |
0.125 |
|
|
|
| 4 |
Cl |
0.125 |
|
|
|
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 |
1.334 |
1.334 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.002 |
0.000 |
0.000 |
| y |
0.000 |
-32.412 |
0.000 |
| z |
0.000 |
0.000 |
-28.685 |
|
| Traceless |
| | x | y | z |
| x |
-1.454 |
0.000 |
0.000 |
| y |
0.000 |
-2.068 |
0.000 |
| z |
0.000 |
0.000 |
3.522 |
|
| Polar |
| 3z2-r2 | 7.044 |
| x2-y2 | 0.410 |
| 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 |
1.599 |
0.000 |
0.000 |
| y |
0.000 |
6.513 |
0.000 |
| z |
0.000 |
0.000 |
3.196 |
<r2> (average value of r
2) Å
2
| <r2> |
105.474 |
| (<r2>)1/2 |
10.270 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31G
| | hartrees |
| Energy at 0K | -958.927653 |
| Energy at 298.15K | -958.928392 |
| HF Energy | -958.927653 |
| Nuclear repulsion energy | 121.553987 |
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 wB97X-D/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' |
3316 |
3316 |
1.20 |
|
|
|
| 2 |
A' |
725 |
725 |
24.74 |
|
|
|
| 3 |
A' |
465 |
465 |
40.20 |
|
|
|
| 4 |
A' |
294 |
294 |
1.14 |
|
|
|
| 5 |
A" |
1253 |
1253 |
45.68 |
|
|
|
| 6 |
A" |
867 |
867 |
174.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3459.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3459.6 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 wB97X-D/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.724 |
0.000 |
| H2 |
-0.471 |
1.690 |
0.000 |
| Cl3 |
0.012 |
-0.177 |
1.522 |
| Cl4 |
0.012 |
-0.177 |
-1.522 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0798 | 1.7685 | 1.7685 |
H2 | 1.0798 | | 2.4565 | 2.4565 | Cl3 | 1.7685 | 2.4565 | | 3.0435 | Cl4 | 1.7685 | 2.4565 | 3.0435 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.113 |
|
Cl3 |
C1 |
Cl4 |
118.733 |
| Cl4 |
C1 |
H2 |
117.113 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.477 |
|
|
|
| 2 |
H |
0.256 |
|
|
|
| 3 |
Cl |
0.110 |
|
|
|
| 4 |
Cl |
0.110 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.659 |
1.251 |
0.000 |
1.415 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.708 |
-1.033 |
0.000 |
| y |
-1.033 |
-29.180 |
0.000 |
| z |
0.000 |
0.000 |
-32.656 |
|
| Traceless |
| | x | y | z |
| x |
-0.791 |
-1.033 |
0.000 |
| y |
-1.033 |
3.002 |
0.000 |
| z |
0.000 |
0.000 |
-2.212 |
|
| Polar |
| 3z2-r2 | -4.423 |
| x2-y2 | -2.528 |
| xy | -1.033 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.689 |
-0.202 |
0.000 |
| y |
-0.202 |
3.220 |
0.000 |
| z |
0.000 |
0.000 |
6.600 |
<r2> (average value of r
2) Å
2
| <r2> |
105.503 |
| (<r2>)1/2 |
10.271 |