Jump to
S1C2
Energy calculated at wB97X-D/STO-3G
| | hartrees |
| Energy at 0K | -948.524554 |
| Energy at 298.15K | |
| HF Energy | -948.524554 |
| Nuclear repulsion energy | 121.074551 |
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/STO-3G
| 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 |
3507 |
3507 |
11.36 |
|
|
|
| 2 |
A1 |
775 |
775 |
24.40 |
|
|
|
| 3 |
A1 |
296 |
296 |
3.01 |
|
|
|
| 4 |
B1 |
531i |
531i |
38.46 |
|
|
|
| 5 |
B2 |
1284 |
1284 |
90.92 |
|
|
|
| 6 |
B2 |
1008 |
1008 |
85.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3169.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3169.5 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/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.699 |
| H2 |
0.000 |
0.000 |
1.797 |
| Cl3 |
0.000 |
1.534 |
-0.176 |
| Cl4 |
0.000 |
-1.534 |
-0.176 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0981 | 1.7659 | 1.7659 |
H2 | 1.0981 | | 2.4992 | 2.4992 | Cl3 | 1.7659 | 2.4992 | | 3.0677 | Cl4 | 1.7659 | 2.4992 | 3.0677 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.705 |
|
Cl3 |
C1 |
Cl4 |
120.590 |
| Cl4 |
C1 |
H2 |
119.705 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.024 |
|
|
|
| 2 |
H |
0.135 |
|
|
|
| 3 |
Cl |
-0.055 |
|
|
|
| 4 |
Cl |
-0.055 |
|
|
|
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 |
1.425 |
1.425 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.130 |
0.000 |
0.000 |
| y |
0.000 |
-31.443 |
0.000 |
| z |
0.000 |
0.000 |
-26.954 |
|
| Traceless |
| | x | y | z |
| x |
0.069 |
0.000 |
0.000 |
| y |
0.000 |
-3.401 |
0.000 |
| z |
0.000 |
0.000 |
3.333 |
|
| Polar |
| 3z2-r2 | 6.666 |
| x2-y2 | 2.313 |
| 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 |
0.450 |
0.000 |
0.000 |
| y |
0.000 |
3.743 |
0.000 |
| z |
0.000 |
0.000 |
1.486 |
<r2> (average value of r
2) Å
2
| <r2> |
105.428 |
| (<r2>)1/2 |
10.268 |
Jump to
S1C1
Energy calculated at wB97X-D/STO-3G
| | hartrees |
| Energy at 0K | -948.527743 |
| Energy at 298.15K | -948.528524 |
| HF Energy | -948.527743 |
| Nuclear repulsion energy | 120.940992 |
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/STO-3G
| 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' |
3429 |
3429 |
5.79 |
|
|
|
| 2 |
A' |
799 |
799 |
32.05 |
|
|
|
| 3 |
A' |
641 |
641 |
3.16 |
|
|
|
| 4 |
A' |
294 |
294 |
2.30 |
|
|
|
| 5 |
A" |
1302 |
1302 |
57.91 |
|
|
|
| 6 |
A" |
968 |
968 |
121.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3716.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3716.0 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/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.016 |
0.747 |
0.000 |
| H2 |
-0.656 |
1.626 |
0.000 |
| Cl3 |
0.016 |
-0.180 |
1.523 |
| Cl4 |
0.016 |
-0.180 |
-1.523 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.1069 | 1.7829 | 1.7829 |
H2 | 1.1069 | | 2.4563 | 2.4563 | Cl3 | 1.7829 | 2.4563 | | 3.0464 | Cl4 | 1.7829 | 2.4563 | 3.0464 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
114.381 |
|
Cl3 |
C1 |
Cl4 |
117.368 |
| Cl4 |
C1 |
H2 |
114.381 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.003 |
|
|
|
| 2 |
H |
0.131 |
|
|
|
| 3 |
Cl |
-0.067 |
|
|
|
| 4 |
Cl |
-0.067 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.571 |
1.358 |
0.000 |
1.473 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.758 |
-0.785 |
0.000 |
| y |
-0.785 |
-27.481 |
0.000 |
| z |
0.000 |
0.000 |
-31.661 |
|
| Traceless |
| | x | y | z |
| x |
0.813 |
-0.785 |
0.000 |
| y |
-0.785 |
2.729 |
0.000 |
| z |
0.000 |
0.000 |
-3.542 |
|
| Polar |
| 3z2-r2 | -7.083 |
| x2-y2 | -1.277 |
| xy | -0.785 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.539 |
-0.206 |
0.000 |
| y |
-0.206 |
1.512 |
0.000 |
| z |
0.000 |
0.000 |
3.866 |
<r2> (average value of r
2) Å
2
| <r2> |
104.716 |
| (<r2>)1/2 |
10.233 |