Jump to
S1C2
Energy calculated at mPW1PW91/6-31G**
| | hartrees |
| Energy at 0K | -959.040891 |
| Energy at 298.15K | |
| HF Energy | -959.040891 |
| Nuclear repulsion energy | 125.813484 |
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 |
3309 |
3148 |
0.20 |
|
|
|
| 2 |
A1 |
772 |
734 |
10.72 |
|
|
|
| 3 |
A1 |
319 |
303 |
0.43 |
|
|
|
| 4 |
B1 |
327i |
311i |
57.32 |
|
|
|
| 5 |
B2 |
1266 |
1205 |
54.79 |
|
|
|
| 6 |
B2 |
950 |
904 |
157.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3144.2 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 2991.7 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 mPW1PW91/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.668 |
| H2 |
0.000 |
0.000 |
1.746 |
| Cl3 |
0.000 |
1.476 |
-0.169 |
| Cl4 |
0.000 |
-1.476 |
-0.169 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0781 | 1.6968 | 1.6968 |
H2 | 1.0781 | | 2.4180 | 2.4180 | Cl3 | 1.6968 | 2.4180 | | 2.9519 | Cl4 | 1.6968 | 2.4180 | 2.9519 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.562 |
|
Cl3 |
C1 |
Cl4 |
120.877 |
| Cl4 |
C1 |
H2 |
119.562 |
|
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 |
-0.357 |
|
|
|
| 2 |
H |
0.220 |
|
|
|
| 3 |
Cl |
0.069 |
|
|
|
| 4 |
Cl |
0.069 |
|
|
|
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 |
1.017 |
1.017 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.639 |
0.000 |
0.000 |
| y |
0.000 |
-30.874 |
0.000 |
| z |
0.000 |
0.000 |
-28.585 |
|
| Traceless |
| | x | y | z |
| x |
-1.910 |
0.000 |
0.000 |
| y |
0.000 |
-0.762 |
0.000 |
| z |
0.000 |
0.000 |
2.672 |
|
| Polar |
| 3z2-r2 | 5.344 |
| x2-y2 | -0.765 |
| 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 |
2.257 |
0.000 |
0.000 |
| y |
0.000 |
6.455 |
0.000 |
| z |
0.000 |
0.000 |
3.632 |
<r2> (average value of r
2) Å
2
| <r2> |
99.732 |
| (<r2>)1/2 |
9.987 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-31G**
| | hartrees |
| Energy at 0K | -959.041398 |
| Energy at 298.15K | -959.042172 |
| HF Energy | -959.041398 |
| Nuclear repulsion energy | 125.688148 |
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' |
3276 |
3117 |
1.37 |
|
|
|
| 2 |
A' |
776 |
739 |
15.34 |
|
|
|
| 3 |
A' |
442 |
420 |
33.21 |
|
|
|
| 4 |
A' |
311 |
296 |
1.40 |
|
|
|
| 5 |
A" |
1270 |
1209 |
47.13 |
|
|
|
| 6 |
A" |
925 |
880 |
178.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3499.6 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 3329.9 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 mPW1PW91/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.687 |
0.000 |
| H2 |
-0.436 |
1.671 |
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 | | 1.0808 | 1.7042 | 1.7042 |
H2 | 1.0808 | | 2.3997 | 2.3997 | Cl3 | 1.7042 | 2.3997 | | 2.9461 | Cl4 | 1.7042 | 2.3997 | 2.9461 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.244 |
|
Cl3 |
C1 |
Cl4 |
119.618 |
| Cl4 |
C1 |
H2 |
117.244 |
|
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 |
-0.339 |
|
|
|
| 2 |
H |
0.217 |
|
|
|
| 3 |
Cl |
0.061 |
|
|
|
| 4 |
Cl |
0.061 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.485 |
0.939 |
0.000 |
1.057 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.404 |
-0.846 |
0.000 |
| y |
-0.846 |
-28.969 |
0.000 |
| z |
0.000 |
0.000 |
-31.008 |
|
| Traceless |
| | x | y | z |
| x |
-1.415 |
-0.846 |
0.000 |
| y |
-0.846 |
2.237 |
0.000 |
| z |
0.000 |
0.000 |
-0.822 |
|
| Polar |
| 3z2-r2 | -1.643 |
| x2-y2 | -2.435 |
| xy | -0.846 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.339 |
-0.181 |
0.000 |
| y |
-0.181 |
3.631 |
0.000 |
| z |
0.000 |
0.000 |
6.516 |
<r2> (average value of r
2) Å
2
| <r2> |
99.604 |
| (<r2>)1/2 |
9.980 |