Jump to
S1C2
Energy calculated at BLYP/6-31+G**
| | hartrees |
| Energy at 0K | -958.987683 |
| Energy at 298.15K | |
| HF Energy | -958.987683 |
| Nuclear repulsion energy | 123.604029 |
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 BLYP/6-31+G**
| 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 |
3195 |
3178 |
0.15 |
|
|
|
| 2 |
A1 |
711 |
707 |
7.19 |
|
|
|
| 3 |
A1 |
300 |
298 |
0.16 |
|
|
|
| 4 |
B1 |
366i |
364i |
59.40 |
|
|
|
| 5 |
B2 |
1207 |
1200 |
46.98 |
|
|
|
| 6 |
B2 |
851 |
847 |
183.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2948.4 cm
-1
Scaled (by 0.9947) Zero Point Vibrational Energy (zpe) 2932.8 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 BLYP/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.678 |
| H2 |
0.000 |
0.000 |
1.764 |
| Cl3 |
0.000 |
1.504 |
-0.171 |
| Cl4 |
0.000 |
-1.504 |
-0.171 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0866 | 1.7271 | 1.7271 |
H2 | 1.0866 | | 2.4513 | 2.4513 | Cl3 | 1.7271 | 2.4513 | | 3.0082 | Cl4 | 1.7271 | 2.4513 | 3.0082 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.442 |
|
Cl3 |
C1 |
Cl4 |
121.116 |
| Cl4 |
C1 |
H2 |
119.442 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.330 |
|
|
|
| 2 |
H |
0.211 |
|
|
|
| 3 |
Cl |
0.060 |
|
|
|
| 4 |
Cl |
0.060 |
|
|
|
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 |
0.908 |
0.908 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.512 |
0.000 |
0.000 |
| y |
0.000 |
-31.469 |
0.000 |
| z |
0.000 |
0.000 |
-29.525 |
|
| Traceless |
| | x | y | z |
| x |
-2.015 |
0.000 |
0.000 |
| y |
0.000 |
-0.450 |
0.000 |
| z |
0.000 |
0.000 |
2.465 |
|
| Polar |
| 3z2-r2 | 4.929 |
| x2-y2 | -1.043 |
| 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 |
3.596 |
0.000 |
0.000 |
| y |
0.000 |
7.881 |
0.000 |
| z |
0.000 |
0.000 |
4.662 |
<r2> (average value of r
2) Å
2
| <r2> |
103.251 |
| (<r2>)1/2 |
10.161 |
Jump to
S1C1
Energy calculated at BLYP/6-31+G**
| | hartrees |
| Energy at 0K | -958.988623 |
| Energy at 298.15K | -958.989345 |
| HF Energy | -958.988623 |
| Nuclear repulsion energy | 123.320218 |
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 BLYP/6-31+G**
| 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' |
3148 |
3131 |
1.12 |
|
|
|
| 2 |
A' |
721 |
717 |
14.37 |
|
|
|
| 3 |
A' |
470 |
467 |
27.17 |
|
|
|
| 4 |
A' |
293 |
292 |
0.34 |
|
|
|
| 5 |
A" |
1211 |
1205 |
37.92 |
|
|
|
| 6 |
A" |
811 |
806 |
213.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3326.5 cm
-1
Scaled (by 0.9947) Zero Point Vibrational Energy (zpe) 3308.8 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 BLYP/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.705 |
0.000 |
| H2 |
-0.514 |
1.660 |
0.000 |
| Cl3 |
0.013 |
-0.173 |
1.501 |
| Cl4 |
0.013 |
-0.173 |
-1.501 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0903 | 1.7394 | 1.7394 |
H2 | 1.0903 | | 2.4274 | 2.4274 | Cl3 | 1.7394 | 2.4274 | | 3.0025 | Cl4 | 1.7394 | 2.4274 | 3.0025 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.251 |
|
Cl3 |
C1 |
Cl4 |
119.328 |
| Cl4 |
C1 |
H2 |
116.251 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.311 |
|
|
|
| 2 |
H |
0.207 |
|
|
|
| 3 |
Cl |
0.052 |
|
|
|
| 4 |
Cl |
0.052 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.560 |
0.814 |
0.000 |
0.988 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.181 |
-1.039 |
0.000 |
| y |
-1.039 |
-30.029 |
0.000 |
| z |
0.000 |
0.000 |
-31.662 |
|
| Traceless |
| | x | y | z |
| x |
-1.335 |
-1.039 |
0.000 |
| y |
-1.039 |
1.893 |
0.000 |
| z |
0.000 |
0.000 |
-0.558 |
|
| Polar |
| 3z2-r2 | -1.115 |
| x2-y2 | -2.152 |
| xy | -1.039 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.671 |
-0.072 |
0.000 |
| y |
-0.072 |
4.731 |
0.000 |
| z |
0.000 |
0.000 |
8.047 |
<r2> (average value of r
2) Å
2
| <r2> |
103.204 |
| (<r2>)1/2 |
10.159 |