Jump to
S1C2
Energy calculated at mPW1PW91/6-31G*
| | hartrees |
| Energy at 0K | -959.039417 |
| Energy at 298.15K | |
| HF Energy | -959.039417 |
| Nuclear repulsion energy | 125.793569 |
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 mPW1PW91/6-31G*
| 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 |
3318 |
3146 |
0.10 |
|
|
|
| 2 |
A1 |
772 |
732 |
10.61 |
|
|
|
| 3 |
A1 |
319 |
302 |
0.42 |
|
|
|
| 4 |
B1 |
335i |
317i |
59.31 |
|
|
|
| 5 |
B2 |
1277 |
1211 |
55.80 |
|
|
|
| 6 |
B2 |
951 |
902 |
157.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3151.2 cm
-1
Scaled (by 0.9483) Zero Point Vibrational Energy (zpe) 2988.3 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 mPW1PW91/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.667 |
| H2 |
0.000 |
0.000 |
1.745 |
| Cl3 |
0.000 |
1.477 |
-0.169 |
| Cl4 |
0.000 |
-1.477 |
-0.169 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0785 | 1.6968 | 1.6968 |
H2 | 1.0785 | | 2.4177 | 2.4177 | Cl3 | 1.6968 | 2.4177 | | 2.9532 | Cl4 | 1.6968 | 2.4177 | 2.9532 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.515 |
|
Cl3 |
C1 |
Cl4 |
120.970 |
| Cl4 |
C1 |
H2 |
119.515 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.399 |
|
|
|
| 2 |
H |
0.259 |
|
|
|
| 3 |
Cl |
0.070 |
|
|
|
| 4 |
Cl |
0.070 |
|
|
|
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 |
1.020 |
1.020 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.654 |
0.000 |
0.000 |
| y |
0.000 |
-30.867 |
0.000 |
| z |
0.000 |
0.000 |
-28.581 |
|
| Traceless |
| | x | y | z |
| x |
-1.930 |
0.000 |
0.000 |
| y |
0.000 |
-0.750 |
0.000 |
| z |
0.000 |
0.000 |
2.679 |
|
| Polar |
| 3z2-r2 | 5.359 |
| x2-y2 | -0.787 |
| 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 |
2.245 |
0.000 |
0.000 |
| y |
0.000 |
6.446 |
0.000 |
| z |
0.000 |
0.000 |
3.612 |
<r2> (average value of r
2) Å
2
| <r2> |
99.783 |
| (<r2>)1/2 |
9.989 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-31G*
| | hartrees |
| Energy at 0K | -959.039970 |
| Energy at 298.15K | -959.040750 |
| HF Energy | -959.039970 |
| Nuclear repulsion energy | 125.669062 |
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 mPW1PW91/6-31G*
| 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' |
3285 |
3115 |
1.61 |
|
|
|
| 2 |
A' |
778 |
737 |
15.57 |
|
|
|
| 3 |
A' |
452 |
429 |
33.35 |
|
|
|
| 4 |
A' |
311 |
295 |
1.31 |
|
|
|
| 5 |
A" |
1283 |
1216 |
47.91 |
|
|
|
| 6 |
A" |
925 |
877 |
179.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3516.4 cm
-1
Scaled (by 0.9483) Zero Point Vibrational Energy (zpe) 3334.6 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 mPW1PW91/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.687 |
0.000 |
| H2 |
-0.444 |
1.667 |
0.000 |
| Cl3 |
0.011 |
-0.170 |
1.473 |
| Cl4 |
0.011 |
-0.170 |
-1.473 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0811 | 1.7045 | 1.7045 |
H2 | 1.0811 | | 2.3988 | 2.3988 | Cl3 | 1.7045 | 2.3988 | | 2.9468 | Cl4 | 1.7045 | 2.3988 | 2.9468 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.126 |
|
Cl3 |
C1 |
Cl4 |
119.638 |
| Cl4 |
C1 |
H2 |
117.126 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.380 |
|
|
|
| 2 |
H |
0.255 |
|
|
|
| 3 |
Cl |
0.063 |
|
|
|
| 4 |
Cl |
0.063 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.499 |
0.937 |
0.000 |
1.062 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.407 |
-0.866 |
0.000 |
| y |
-0.866 |
-28.985 |
0.000 |
| z |
0.000 |
0.000 |
-31.007 |
|
| Traceless |
| | x | y | z |
| x |
-1.411 |
-0.866 |
0.000 |
| y |
-0.866 |
2.222 |
0.000 |
| z |
0.000 |
0.000 |
-0.810 |
|
| Polar |
| 3z2-r2 | -1.621 |
| x2-y2 | -2.422 |
| xy | -0.866 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.329 |
-0.182 |
0.000 |
| y |
-0.182 |
3.613 |
0.000 |
| z |
0.000 |
0.000 |
6.508 |
<r2> (average value of r
2) Å
2
| <r2> |
99.637 |
| (<r2>)1/2 |
9.982 |