Jump to
S1C2
Energy calculated at BLYP/6-31G**
| | hartrees |
| Energy at 0K | -958.981536 |
| Energy at 298.15K | |
| HF Energy | -958.981536 |
| Nuclear repulsion energy | 123.638548 |
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/6-31G**
| 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 |
3200 |
3175 |
0.00 |
|
|
|
| 2 |
A1 |
713 |
708 |
9.22 |
|
|
|
| 3 |
A1 |
300 |
297 |
0.28 |
|
|
|
| 4 |
B1 |
377i |
374i |
57.80 |
|
|
|
| 5 |
B2 |
1208 |
1199 |
49.05 |
|
|
|
| 6 |
B2 |
856 |
850 |
171.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2949.8 cm
-1
Scaled (by 0.9923) Zero Point Vibrational Energy (zpe) 2927.1 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/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.677 |
| H2 |
0.000 |
0.000 |
1.763 |
| Cl3 |
0.000 |
1.504 |
-0.171 |
| Cl4 |
0.000 |
-1.504 |
-0.171 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0860 | 1.7267 | 1.7267 |
H2 | 1.0860 | | 2.4504 | 2.4504 | Cl3 | 1.7267 | 2.4504 | | 3.0073 | Cl4 | 1.7267 | 2.4504 | 3.0073 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.444 |
|
Cl3 |
C1 |
Cl4 |
121.111 |
| Cl4 |
C1 |
H2 |
119.444 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.290 |
|
|
|
| 2 |
H |
0.174 |
|
|
|
| 3 |
Cl |
0.058 |
|
|
|
| 4 |
Cl |
0.058 |
|
|
|
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 |
0.929 |
0.929 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.685 |
0.000 |
0.000 |
| y |
0.000 |
-30.774 |
0.000 |
| z |
0.000 |
0.000 |
-28.790 |
|
| Traceless |
| | x | y | z |
| x |
-1.904 |
0.000 |
0.000 |
| y |
0.000 |
-0.536 |
0.000 |
| z |
0.000 |
0.000 |
2.440 |
|
| Polar |
| 3z2-r2 | 4.880 |
| x2-y2 | -0.911 |
| 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 |
2.282 |
0.000 |
0.000 |
| y |
0.000 |
6.973 |
0.000 |
| z |
0.000 |
0.000 |
3.750 |
<r2> (average value of r
2) Å
2
| <r2> |
102.734 |
| (<r2>)1/2 |
10.136 |
Jump to
S1C1
Energy calculated at BLYP/6-31G**
| | hartrees |
| Energy at 0K | -958.982590 |
| Energy at 298.15K | -958.983322 |
| HF Energy | -958.982590 |
| Nuclear repulsion energy | 123.331653 |
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/6-31G**
| 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' |
3149 |
3125 |
2.74 |
|
|
|
| 2 |
A' |
725 |
720 |
17.29 |
|
|
|
| 3 |
A' |
482 |
478 |
25.38 |
|
|
|
| 4 |
A' |
294 |
291 |
0.35 |
|
|
|
| 5 |
A" |
1212 |
1202 |
38.90 |
|
|
|
| 6 |
A" |
814 |
808 |
200.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3337.3 cm
-1
Scaled (by 0.9923) Zero Point Vibrational Energy (zpe) 3311.6 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 BLYP/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.707 |
0.000 |
| H2 |
-0.528 |
1.653 |
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 | | 1.0901 | 1.7399 | 1.7399 |
H2 | 1.0901 | | 2.4252 | 2.4252 | Cl3 | 1.7399 | 2.4252 | | 3.0014 | Cl4 | 1.7399 | 2.4252 | 3.0014 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.056 |
|
Cl3 |
C1 |
Cl4 |
119.203 |
| Cl4 |
C1 |
H2 |
116.056 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.270 |
|
|
|
| 2 |
H |
0.174 |
|
|
|
| 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 |
| |
-0.569 |
0.823 |
0.000 |
1.001 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.375 |
-0.940 |
0.000 |
| y |
-0.940 |
-29.308 |
0.000 |
| z |
0.000 |
0.000 |
-30.974 |
|
| Traceless |
| | x | y | z |
| x |
-1.234 |
-0.940 |
0.000 |
| y |
-0.940 |
1.867 |
0.000 |
| z |
0.000 |
0.000 |
-0.633 |
|
| Polar |
| 3z2-r2 | -1.266 |
| x2-y2 | -2.067 |
| xy | -0.940 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.407 |
-0.230 |
0.000 |
| y |
-0.230 |
3.760 |
0.000 |
| z |
0.000 |
0.000 |
7.111 |
<r2> (average value of r
2) Å
2
| <r2> |
102.693 |
| (<r2>)1/2 |
10.134 |