Jump to
S1C2
Energy calculated at wB97X-D/SDD
| | hartrees |
| Energy at 0K | -958.926033 |
| Energy at 298.15K | |
| HF Energy | -958.926033 |
| Nuclear repulsion energy | 121.361613 |
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/SDD
| 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 |
3346 |
3346 |
0.41 |
|
|
|
| 2 |
A1 |
702 |
702 |
16.62 |
|
|
|
| 3 |
A1 |
293 |
293 |
0.68 |
|
|
|
| 4 |
B1 |
419i |
419i |
111.61 |
|
|
|
| 5 |
B2 |
1224 |
1224 |
44.64 |
|
|
|
| 6 |
B2 |
886 |
886 |
160.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3015.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3015.9 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 wB97X-D/SDD
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.703 |
| H2 |
0.000 |
0.000 |
1.781 |
| Cl3 |
0.000 |
1.530 |
-0.176 |
| Cl4 |
0.000 |
-1.530 |
-0.176 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0782 | 1.7644 | 1.7644 |
H2 | 1.0782 | | 2.4843 | 2.4843 | Cl3 | 1.7644 | 2.4843 | | 3.0592 | Cl4 | 1.7644 | 2.4843 | 3.0592 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.894 |
|
Cl3 |
C1 |
Cl4 |
120.213 |
| Cl4 |
C1 |
H2 |
119.894 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/SDD
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.399 |
|
|
|
| 2 |
H |
0.304 |
|
|
|
| 3 |
Cl |
0.048 |
|
|
|
| 4 |
Cl |
0.048 |
|
|
|
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 |
1.308 |
1.308 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.104 |
0.000 |
0.000 |
| y |
0.000 |
-32.384 |
0.000 |
| z |
0.000 |
0.000 |
-28.673 |
|
| Traceless |
| | x | y | z |
| x |
-1.575 |
0.000 |
0.000 |
| y |
0.000 |
-1.996 |
0.000 |
| z |
0.000 |
0.000 |
3.571 |
|
| Polar |
| 3z2-r2 | 7.142 |
| x2-y2 | 0.280 |
| 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 |
1.430 |
0.000 |
0.000 |
| y |
0.000 |
6.158 |
0.000 |
| z |
0.000 |
0.000 |
2.935 |
<r2> (average value of r
2) Å
2
| <r2> |
106.142 |
| (<r2>)1/2 |
10.303 |
Jump to
S1C1
Energy calculated at wB97X-D/SDD
| | hartrees |
| Energy at 0K | -958.927305 |
| Energy at 298.15K | -958.928062 |
| HF Energy | -958.927305 |
| Nuclear repulsion energy | 121.096767 |
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/SDD
| 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' |
3294 |
3294 |
3.15 |
|
|
|
| 2 |
A' |
717 |
717 |
29.78 |
|
|
|
| 3 |
A' |
515 |
515 |
28.50 |
|
|
|
| 4 |
A' |
288 |
288 |
0.86 |
|
|
|
| 5 |
A" |
1245 |
1245 |
36.58 |
|
|
|
| 6 |
A" |
847 |
847 |
183.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3452.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3452.9 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 wB97X-D/SDD
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.734 |
0.000 |
| H2 |
-0.540 |
1.665 |
0.000 |
| Cl3 |
0.013 |
-0.178 |
1.526 |
| Cl4 |
0.013 |
-0.178 |
-1.526 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0826 | 1.7778 | 1.7778 |
H2 | 1.0826 | | 2.4558 | 2.4558 | Cl3 | 1.7778 | 2.4558 | | 3.0516 | Cl4 | 1.7778 | 2.4558 | 3.0516 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.182 |
|
Cl3 |
C1 |
Cl4 |
118.241 |
| Cl4 |
C1 |
H2 |
116.182 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/SDD
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.354 |
|
|
|
| 2 |
H |
0.289 |
|
|
|
| 3 |
Cl |
0.033 |
|
|
|
| 4 |
Cl |
0.033 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.768 |
1.207 |
0.000 |
1.431 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.691 |
-1.193 |
0.000 |
| y |
-1.193 |
-29.274 |
0.000 |
| z |
0.000 |
0.000 |
-32.707 |
|
| Traceless |
| | x | y | z |
| x |
-0.700 |
-1.193 |
0.000 |
| y |
-1.193 |
2.924 |
0.000 |
| z |
0.000 |
0.000 |
-2.225 |
|
| Polar |
| 3z2-r2 | -4.449 |
| x2-y2 | -2.416 |
| xy | -1.193 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.511 |
-0.159 |
0.000 |
| y |
-0.159 |
3.021 |
0.000 |
| z |
0.000 |
0.000 |
6.231 |
<r2> (average value of r
2) Å
2
| <r2> |
106.040 |
| (<r2>)1/2 |
10.298 |