Jump to
S1C2
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -959.048498 |
| Energy at 298.15K | |
| HF Energy | -959.048498 |
| Nuclear repulsion energy | 125.594024 |
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 |
3287 |
3144 |
0.00 |
|
|
|
| 2 |
A1 |
763 |
730 |
9.36 |
|
|
|
| 3 |
A1 |
318 |
304 |
0.20 |
|
|
|
| 4 |
B1 |
363i |
348i |
61.29 |
|
|
|
| 5 |
B2 |
1248 |
1194 |
50.51 |
|
|
|
| 6 |
B2 |
931 |
890 |
173.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3091.6 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 2957.1 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 C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.672 |
| H2 |
0.000 |
0.000 |
1.749 |
| Cl3 |
0.000 |
1.478 |
-0.170 |
| Cl4 |
0.000 |
-1.478 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0768 | 1.7009 | 1.7009 |
H2 | 1.0768 | | 2.4222 | 2.4222 | Cl3 | 1.7009 | 2.4222 | | 2.9552 | Cl4 | 1.7009 | 2.4222 | 2.9552 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.689 |
|
Cl3 |
C1 |
Cl4 |
120.622 |
| Cl4 |
C1 |
H2 |
119.689 |
|
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 |
-0.297 |
|
|
|
| 2 |
H |
0.224 |
|
|
|
| 3 |
Cl |
0.037 |
|
|
|
| 4 |
Cl |
0.037 |
|
|
|
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 |
1.004 |
1.004 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.346 |
0.000 |
0.000 |
| y |
0.000 |
-31.493 |
0.000 |
| z |
0.000 |
0.000 |
-29.203 |
|
| Traceless |
| | x | y | z |
| x |
-1.998 |
0.000 |
0.000 |
| y |
0.000 |
-0.718 |
0.000 |
| z |
0.000 |
0.000 |
2.716 |
|
| Polar |
| 3z2-r2 | 5.432 |
| x2-y2 | -0.853 |
| 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 |
2.206 |
0.000 |
0.000 |
| y |
0.000 |
6.865 |
0.000 |
| z |
0.000 |
0.000 |
3.645 |
<r2> (average value of r
2) Å
2
| <r2> |
100.360 |
| (<r2>)1/2 |
10.018 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -959.049129 |
| Energy at 298.15K | -959.049937 |
| HF Energy | -959.049129 |
| Nuclear repulsion energy | 125.440311 |
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' |
3255 |
3114 |
1.67 |
|
|
|
| 2 |
A' |
768 |
735 |
14.84 |
|
|
|
| 3 |
A' |
481 |
460 |
33.59 |
|
|
|
| 4 |
A' |
312 |
298 |
0.75 |
|
|
|
| 5 |
A" |
1257 |
1202 |
43.87 |
|
|
|
| 6 |
A" |
903 |
864 |
197.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3488.1 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 3336.4 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 |
-0.460 |
1.665 |
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 | | 1.0798 | 1.7095 | 1.7095 |
H2 | 1.0798 | | 2.4017 | 2.4017 | Cl3 | 1.7095 | 2.4017 | | 2.9490 | Cl4 | 1.7095 | 2.4017 | 2.9490 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.073 |
|
Cl3 |
C1 |
Cl4 |
119.211 |
| Cl4 |
C1 |
H2 |
117.073 |
|
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 |
-0.278 |
|
|
|
| 2 |
H |
0.220 |
|
|
|
| 3 |
Cl |
0.029 |
|
|
|
| 4 |
Cl |
0.029 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.523 |
0.921 |
0.000 |
1.059 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.074 |
-0.902 |
0.000 |
| y |
-0.902 |
-29.624 |
0.000 |
| z |
0.000 |
0.000 |
-31.661 |
|
| Traceless |
| | x | y | z |
| x |
-1.431 |
-0.902 |
0.000 |
| y |
-0.902 |
2.244 |
0.000 |
| z |
0.000 |
0.000 |
-0.812 |
|
| Polar |
| 3z2-r2 | -1.625 |
| x2-y2 | -2.450 |
| xy | -0.902 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.284 |
-0.152 |
0.000 |
| y |
-0.152 |
3.669 |
0.000 |
| z |
0.000 |
0.000 |
6.933 |
<r2> (average value of r
2) Å
2
| <r2> |
100.232 |
| (<r2>)1/2 |
10.012 |