Jump to
S1C2
Energy calculated at ROHF/6-31G**
| | hartrees |
| Energy at 0K | -957.352579 |
| Energy at 298.15K | |
| HF Energy | -957.352579 |
| Nuclear repulsion energy | 125.702825 |
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 ROHF/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 |
3462 |
2958 |
0.08 |
|
|
|
| 2 |
A1 |
800 |
684 |
14.75 |
|
|
|
| 3 |
A1 |
331 |
283 |
1.05 |
|
|
|
| 4 |
B1 |
605i |
517i |
45.77 |
|
|
|
| 5 |
B2 |
1359 |
1161 |
78.06 |
|
|
|
| 6 |
B2 |
1006 |
859 |
122.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3176.2 cm
-1
Scaled (by 0.8546) Zero Point Vibrational Energy (zpe) 2714.4 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 ROHF/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.675 |
| H2 |
0.000 |
0.000 |
1.741 |
| Cl3 |
0.000 |
1.476 |
-0.170 |
| Cl4 |
0.000 |
-1.476 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0660 | 1.7009 | 1.7009 |
H2 | 1.0660 | | 2.4150 | 2.4150 | Cl3 | 1.7009 | 2.4150 | | 2.9519 | Cl4 | 1.7009 | 2.4150 | 2.9519 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.804 |
|
Cl3 |
C1 |
Cl4 |
120.392 |
| Cl4 |
C1 |
H2 |
119.804 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.281 |
|
|
|
| 2 |
H |
0.219 |
|
|
|
| 3 |
Cl |
0.031 |
|
|
|
| 4 |
Cl |
0.031 |
|
|
|
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 |
1.291 |
1.291 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.090 |
0.000 |
0.000 |
| y |
0.000 |
-32.086 |
-0.000 |
| z |
0.000 |
-0.000 |
-28.895 |
|
| Traceless |
| | x | y | z |
| x |
-1.599 |
0.000 |
0.000 |
| y |
0.000 |
-1.594 |
-0.000 |
| z |
0.000 |
-0.000 |
3.193 |
|
| Polar |
| 3z2-r2 | 6.387 |
| x2-y2 | -0.003 |
| 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 |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
100.196 |
| (<r2>)1/2 |
10.010 |
Jump to
S1C1
Energy calculated at ROHF/6-31G**
| | hartrees |
| Energy at 0K | -957.355372 |
| Energy at 298.15K | -957.356356 |
| HF Energy | -957.355372 |
| Nuclear repulsion energy | 125.454839 |
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 ROHF/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' |
3400 |
2905 |
3.98 |
|
|
|
| 2 |
A' |
823 |
703 |
23.75 |
|
|
|
| 3 |
A' |
687 |
587 |
9.17 |
|
|
|
| 4 |
A' |
326 |
279 |
0.76 |
|
|
|
| 5 |
A" |
1369 |
1170 |
61.46 |
|
|
|
| 6 |
A" |
960 |
821 |
163.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3782.4 cm
-1
Scaled (by 0.8546) Zero Point Vibrational Energy (zpe) 3232.4 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 ROHF/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.014 |
0.709 |
0.000 |
| H2 |
-0.563 |
1.612 |
0.000 |
| Cl3 |
0.014 |
-0.173 |
1.471 |
| Cl4 |
0.014 |
-0.173 |
-1.471 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0711 | 1.7148 | 1.7148 |
H2 | 1.0711 | | 2.3832 | 2.3832 | Cl3 | 1.7148 | 2.3832 | | 2.9416 | Cl4 | 1.7148 | 2.3832 | 2.9416 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
115.674 |
|
Cl3 |
C1 |
Cl4 |
118.116 |
| Cl4 |
C1 |
H2 |
115.674 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.232 |
|
|
|
| 2 |
H |
0.208 |
|
|
|
| 3 |
Cl |
0.012 |
|
|
|
| 4 |
Cl |
0.012 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.545 |
1.214 |
0.000 |
1.330 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.711 |
-0.945 |
0.000 |
| y |
-0.945 |
-29.489 |
-0.000 |
| z |
0.000 |
-0.000 |
-32.407 |
|
| Traceless |
| | x | y | z |
| x |
-0.763 |
-0.945 |
0.000 |
| y |
-0.945 |
2.570 |
-0.000 |
| z |
0.000 |
-0.000 |
-1.807 |
|
| Polar |
| 3z2-r2 | -3.615 |
| x2-y2 | -2.222 |
| xy | -0.945 |
| xz | 0.000 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
99.992 |
| (<r2>)1/2 |
10.000 |