Jump to
S1C2
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -36.039928 |
| Energy at 298.15K | |
| HF Energy | -36.039928 |
| Nuclear repulsion energy | 30.743520 |
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/CEP-121G*
| 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 |
3235 |
3136 |
0.55 |
|
|
|
| 2 |
A1 |
734 |
711 |
10.65 |
|
|
|
| 3 |
A1 |
299 |
290 |
0.30 |
|
|
|
| 4 |
B1 |
414i |
402i |
60.40 |
|
|
|
| 5 |
B2 |
1231 |
1193 |
58.88 |
|
|
|
| 6 |
B2 |
898 |
871 |
169.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2991.2 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 2899.6 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/CEP-121G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.682 |
| H2 |
0.000 |
0.000 |
1.766 |
| Cl3 |
0.000 |
1.503 |
-0.172 |
| Cl4 |
0.000 |
-1.503 |
-0.172 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0832 | 1.7288 | 1.7288 |
H2 | 1.0832 | | 2.4524 | 2.4524 | Cl3 | 1.7288 | 2.4524 | | 3.0054 | Cl4 | 1.7288 | 2.4524 | 3.0054 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.633 |
|
Cl3 |
C1 |
Cl4 |
120.734 |
| Cl4 |
C1 |
H2 |
119.633 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.244 |
|
|
|
| 2 |
H |
0.237 |
|
|
|
| 3 |
Cl |
0.004 |
|
|
|
| 4 |
Cl |
0.004 |
|
|
|
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 |
0.959 |
0.959 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-30.725 |
0.000 |
0.000 |
| y |
0.000 |
-29.569 |
0.000 |
| z |
0.000 |
0.000 |
-27.544 |
|
| Traceless |
| | x | y | z |
| x |
-2.168 |
0.000 |
0.000 |
| y |
0.000 |
-0.435 |
0.000 |
| z |
0.000 |
0.000 |
2.603 |
|
| Polar |
| 3z2-r2 | 5.206 |
| x2-y2 | -1.155 |
| 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 |
2.804 |
0.000 |
0.000 |
| y |
0.000 |
7.159 |
0.000 |
| z |
0.000 |
0.000 |
4.132 |
<r2> (average value of r
2) Å
2
| <r2> |
55.298 |
| (<r2>)1/2 |
7.436 |
Jump to
S1C1
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -36.041252 |
| Energy at 298.15K | -36.042046 |
| HF Energy | -36.041252 |
| Nuclear repulsion energy | 30.680938 |
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/CEP-121G*
| 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' |
3191 |
3093 |
4.68 |
|
|
|
| 2 |
A' |
746 |
723 |
18.95 |
|
|
|
| 3 |
A' |
530 |
514 |
22.44 |
|
|
|
| 4 |
A' |
293 |
284 |
0.38 |
|
|
|
| 5 |
A" |
1240 |
1202 |
49.61 |
|
|
|
| 6 |
A" |
858 |
832 |
202.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3428.7 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 3323.7 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/CEP-121G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.014 |
0.713 |
0.000 |
| H2 |
-0.540 |
1.649 |
0.000 |
| Cl3 |
0.014 |
-0.174 |
1.498 |
| Cl4 |
0.014 |
-0.174 |
-1.498 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0870 | 1.7411 | 1.7411 |
H2 | 1.0870 | | 2.4236 | 2.4236 | Cl3 | 1.7411 | 2.4236 | | 2.9955 | Cl4 | 1.7411 | 2.4236 | 2.9955 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.029 |
|
Cl3 |
C1 |
Cl4 |
118.685 |
| Cl4 |
C1 |
H2 |
116.029 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.202 |
|
|
|
| 2 |
H |
0.222 |
|
|
|
| 3 |
Cl |
-0.010 |
|
|
|
| 4 |
Cl |
-0.010 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.585 |
0.860 |
0.000 |
1.040 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-30.355 |
-1.033 |
0.000 |
| y |
-1.033 |
-28.101 |
0.000 |
| z |
0.000 |
0.000 |
-29.813 |
|
| Traceless |
| | x | y | z |
| x |
-1.398 |
-1.033 |
0.000 |
| y |
-1.033 |
1.983 |
0.000 |
| z |
0.000 |
0.000 |
-0.585 |
|
| Polar |
| 3z2-r2 | -1.170 |
| x2-y2 | -2.254 |
| xy | -1.033 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.917 |
-0.170 |
0.000 |
| y |
-0.170 |
4.170 |
0.000 |
| z |
0.000 |
0.000 |
7.252 |
<r2> (average value of r
2) Å
2
| <r2> |
55.257 |
| (<r2>)1/2 |
7.434 |