Jump to
S1C2
Energy calculated at B3LYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -959.128886 |
| Energy at 298.15K | |
| HF Energy | -959.128886 |
| Nuclear repulsion energy | 125.495703 |
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 B3LYP/aug-cc-pVTZ
| 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 |
3255 |
3150 |
0.67 |
|
|
|
| 2 |
A1 |
740 |
716 |
6.21 |
|
|
|
| 3 |
A1 |
306 |
296 |
0.30 |
|
|
|
| 4 |
B1 |
342i |
331i |
35.03 |
|
|
|
| 5 |
B2 |
1225 |
1186 |
47.74 |
|
|
|
| 6 |
B2 |
894 |
865 |
147.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3038.8 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 2940.0 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 B3LYP/aug-cc-pVTZ
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 |
1.747 |
| Cl3 |
0.000 |
1.479 |
-0.170 |
| Cl4 |
0.000 |
-1.479 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0746 | 1.7022 | 1.7022 |
H2 | 1.0746 | | 2.4211 | 2.4211 | Cl3 | 1.7022 | 2.4211 | | 2.9587 | Cl4 | 1.7022 | 2.4211 | 2.9587 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.647 |
|
Cl3 |
C1 |
Cl4 |
120.705 |
| Cl4 |
C1 |
H2 |
119.647 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.296 |
|
|
|
| 2 |
H |
0.330 |
|
|
|
| 3 |
Cl |
-0.017 |
|
|
|
| 4 |
Cl |
-0.017 |
|
|
|
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 |
0.907 |
0.907 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.092 |
0.000 |
0.000 |
| y |
0.000 |
-31.281 |
0.000 |
| z |
0.000 |
0.000 |
-29.262 |
|
| Traceless |
| | x | y | z |
| x |
-1.821 |
0.000 |
0.000 |
| y |
0.000 |
-0.604 |
0.000 |
| z |
0.000 |
0.000 |
2.425 |
|
| Polar |
| 3z2-r2 | 4.850 |
| x2-y2 | -0.811 |
| 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 |
4.808 |
0.000 |
0.000 |
| y |
0.000 |
8.515 |
0.000 |
| z |
0.000 |
0.000 |
5.647 |
<r2> (average value of r
2) Å
2
| <r2> |
100.436 |
| (<r2>)1/2 |
10.022 |
Jump to
S1C1
Energy calculated at B3LYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -959.129513 |
| Energy at 298.15K | -959.130264 |
| HF Energy | -959.129513 |
| Nuclear repulsion energy | 125.303407 |
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 B3LYP/aug-cc-pVTZ
| 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' |
3221 |
3116 |
0.44 |
|
|
|
| 2 |
A' |
747 |
722 |
10.59 |
|
|
|
| 3 |
A' |
450 |
435 |
22.32 |
|
|
|
| 4 |
A' |
300 |
290 |
0.62 |
|
|
|
| 5 |
A" |
1231 |
1191 |
39.08 |
|
|
|
| 6 |
A" |
864 |
835 |
170.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3405.5 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 3294.9 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 B3LYP/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.694 |
0.000 |
| H2 |
-0.457 |
1.664 |
0.000 |
| Cl3 |
0.011 |
-0.171 |
1.477 |
| Cl4 |
0.011 |
-0.171 |
-1.477 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0774 | 1.7114 | 1.7114 |
H2 | 1.0774 | | 2.4016 | 2.4016 | Cl3 | 1.7114 | 2.4016 | | 2.9532 | Cl4 | 1.7114 | 2.4016 | 2.9532 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.073 |
|
Cl3 |
C1 |
Cl4 |
119.272 |
| Cl4 |
C1 |
H2 |
117.073 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.282 |
|
|
|
| 2 |
H |
0.310 |
|
|
|
| 3 |
Cl |
-0.014 |
|
|
|
| 4 |
Cl |
-0.014 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.411 |
0.831 |
0.000 |
0.927 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.854 |
-0.842 |
0.000 |
| y |
-0.842 |
-29.627 |
0.000 |
| z |
0.000 |
0.000 |
-31.365 |
|
| Traceless |
| | x | y | z |
| x |
-1.358 |
-0.842 |
0.000 |
| y |
-0.842 |
1.983 |
0.000 |
| z |
0.000 |
0.000 |
-0.625 |
|
| Polar |
| 3z2-r2 | -1.250 |
| x2-y2 | -2.227 |
| xy | -0.842 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.846 |
-0.052 |
0.000 |
| y |
-0.052 |
5.681 |
0.000 |
| z |
0.000 |
0.000 |
8.596 |
<r2> (average value of r
2) Å
2
| <r2> |
100.331 |
| (<r2>)1/2 |
10.017 |