Jump to
S1C2
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -959.046650 |
| Energy at 298.15K | |
| HF Energy | -959.046650 |
| Nuclear repulsion energy | 125.568442 |
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/6-311G*
| 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 |
3286 |
3286 |
0.20 |
|
|
|
| 2 |
A1 |
763 |
763 |
9.38 |
|
|
|
| 3 |
A1 |
318 |
318 |
0.20 |
|
|
|
| 4 |
B1 |
374i |
374i |
64.04 |
|
|
|
| 5 |
B2 |
1260 |
1260 |
50.60 |
|
|
|
| 6 |
B2 |
932 |
932 |
172.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3092.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3092.3 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 wB97X-D/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.671 |
| H2 |
0.000 |
0.000 |
1.748 |
| Cl3 |
0.000 |
1.478 |
-0.170 |
| Cl4 |
0.000 |
-1.478 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0774 | 1.7008 | 1.7008 |
H2 | 1.0774 | | 2.4218 | 2.4218 | Cl3 | 1.7008 | 2.4218 | | 2.9569 | Cl4 | 1.7008 | 2.4218 | 2.9569 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.627 |
|
Cl3 |
C1 |
Cl4 |
120.746 |
| Cl4 |
C1 |
H2 |
119.627 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.398 |
|
|
|
| 2 |
H |
0.312 |
|
|
|
| 3 |
Cl |
0.043 |
|
|
|
| 4 |
Cl |
0.043 |
|
|
|
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 |
1.018 |
1.018 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.391 |
0.000 |
0.000 |
| y |
0.000 |
-31.501 |
0.000 |
| z |
0.000 |
0.000 |
-29.162 |
|
| Traceless |
| | x | y | z |
| x |
-2.060 |
0.000 |
0.000 |
| y |
0.000 |
-0.724 |
0.000 |
| z |
0.000 |
0.000 |
2.784 |
|
| Polar |
| 3z2-r2 | 5.568 |
| x2-y2 | -0.890 |
| 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 |
2.180 |
0.000 |
0.000 |
| y |
0.000 |
6.857 |
0.000 |
| z |
0.000 |
0.000 |
3.620 |
<r2> (average value of r
2) Å
2
| <r2> |
100.428 |
| (<r2>)1/2 |
10.021 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -959.047413 |
| Energy at 298.15K | -959.048230 |
| HF Energy | -959.047413 |
| Nuclear repulsion energy | 125.408298 |
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/6-311G*
| 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' |
3253 |
3253 |
2.85 |
|
|
|
| 2 |
A' |
770 |
770 |
15.69 |
|
|
|
| 3 |
A' |
498 |
498 |
33.14 |
|
|
|
| 4 |
A' |
312 |
312 |
0.68 |
|
|
|
| 5 |
A" |
1271 |
1271 |
43.50 |
|
|
|
| 6 |
A" |
902 |
902 |
198.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3503.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3503.1 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.694 |
0.000 |
| H2 |
-0.477 |
1.658 |
0.000 |
| Cl3 |
0.012 |
-0.171 |
1.475 |
| Cl4 |
0.012 |
-0.171 |
-1.475 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0804 | 1.7101 | 1.7101 |
H2 | 1.0804 | | 2.3998 | 2.3998 | Cl3 | 1.7101 | 2.3998 | | 2.9498 | Cl4 | 1.7101 | 2.3998 | 2.9498 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.827 |
|
Cl3 |
C1 |
Cl4 |
119.190 |
| Cl4 |
C1 |
H2 |
116.827 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.377 |
|
|
|
| 2 |
H |
0.305 |
|
|
|
| 3 |
Cl |
0.036 |
|
|
|
| 4 |
Cl |
0.036 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.550 |
0.924 |
0.000 |
1.075 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.086 |
-0.956 |
0.000 |
| y |
-0.956 |
-29.632 |
0.000 |
| z |
0.000 |
0.000 |
-31.681 |
|
| Traceless |
| | x | y | z |
| x |
-1.430 |
-0.956 |
0.000 |
| y |
-0.956 |
2.252 |
0.000 |
| z |
0.000 |
0.000 |
-0.822 |
|
| Polar |
| 3z2-r2 | -1.643 |
| x2-y2 | -2.455 |
| xy | -0.956 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.265 |
-0.159 |
0.000 |
| y |
-0.159 |
3.648 |
0.000 |
| z |
0.000 |
0.000 |
6.928 |
<r2> (average value of r
2) Å
2
| <r2> |
100.275 |
| (<r2>)1/2 |
10.014 |