Jump to
S1C2
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -948.447288 |
| Energy at 298.15K | |
| HF Energy | -948.447288 |
| Nuclear repulsion energy | 120.857884 |
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 B3PW91/STO-3G
| 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 |
3485 |
3084 |
10.85 |
|
|
|
| 2 |
A1 |
776 |
687 |
23.37 |
|
|
|
| 3 |
A1 |
294 |
260 |
2.96 |
|
|
|
| 4 |
B1 |
533i |
472i |
39.95 |
|
|
|
| 5 |
B2 |
1277 |
1130 |
90.99 |
|
|
|
| 6 |
B2 |
1014 |
897 |
87.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3156.3 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 2793.3 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 B3PW91/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.697 |
| H2 |
0.000 |
0.000 |
1.796 |
| Cl3 |
0.000 |
1.538 |
-0.176 |
| Cl4 |
0.000 |
-1.538 |
-0.176 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0988 | 1.7684 | 1.7684 |
H2 | 1.0988 | | 2.5008 | 2.5008 | Cl3 | 1.7684 | 2.5008 | | 3.0753 | Cl4 | 1.7684 | 2.5008 | 3.0753 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.596 |
|
Cl3 |
C1 |
Cl4 |
120.808 |
| Cl4 |
C1 |
H2 |
119.596 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.026 |
|
|
|
| 2 |
H |
0.137 |
|
|
|
| 3 |
Cl |
-0.056 |
|
|
|
| 4 |
Cl |
-0.056 |
|
|
|
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 |
1.405 |
1.405 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.134 |
0.000 |
0.000 |
| y |
0.000 |
-31.304 |
0.000 |
| z |
0.000 |
0.000 |
-26.924 |
|
| Traceless |
| | x | y | z |
| x |
-0.020 |
0.000 |
0.000 |
| y |
0.000 |
-3.274 |
0.000 |
| z |
0.000 |
0.000 |
3.294 |
|
| Polar |
| 3z2-r2 | 6.589 |
| x2-y2 | 2.169 |
| 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 |
0.457 |
0.000 |
0.000 |
| y |
0.000 |
3.859 |
0.000 |
| z |
0.000 |
0.000 |
1.493 |
<r2> (average value of r
2) Å
2
| <r2> |
105.777 |
| (<r2>)1/2 |
10.285 |
Jump to
S1C1
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -948.450723 |
| Energy at 298.15K | -948.451505 |
| HF Energy | -948.450723 |
| Nuclear repulsion energy | 120.723250 |
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 B3PW91/STO-3G
| 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' |
3408 |
3016 |
4.91 |
|
|
|
| 2 |
A' |
802 |
710 |
31.14 |
|
|
|
| 3 |
A' |
651 |
576 |
3.41 |
|
|
|
| 4 |
A' |
289 |
256 |
2.24 |
|
|
|
| 5 |
A" |
1286 |
1138 |
55.58 |
|
|
|
| 6 |
A" |
972 |
860 |
124.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3704.1 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 3278.1 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 B3PW91/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.017 |
0.747 |
0.000 |
| H2 |
-0.669 |
1.618 |
0.000 |
| Cl3 |
0.017 |
-0.179 |
1.527 |
| Cl4 |
0.017 |
-0.179 |
-1.527 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.1078 | 1.7860 | 1.7860 |
H2 | 1.1078 | | 2.4557 | 2.4557 | Cl3 | 1.7860 | 2.4557 | | 3.0533 | Cl4 | 1.7860 | 2.4557 | 3.0533 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
114.060 |
|
Cl3 |
C1 |
Cl4 |
117.475 |
| Cl4 |
C1 |
H2 |
114.060 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.000 |
|
|
|
| 2 |
H |
0.134 |
|
|
|
| 3 |
Cl |
-0.067 |
|
|
|
| 4 |
Cl |
-0.067 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.590 |
1.325 |
0.000 |
1.451 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.740 |
-0.807 |
0.000 |
| y |
-0.807 |
-27.479 |
0.000 |
| z |
0.000 |
0.000 |
-31.516 |
|
| Traceless |
| | x | y | z |
| x |
0.757 |
-0.807 |
0.000 |
| y |
-0.807 |
2.649 |
0.000 |
| z |
0.000 |
0.000 |
-3.406 |
|
| Polar |
| 3z2-r2 | -6.812 |
| x2-y2 | -1.261 |
| xy | -0.807 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.549 |
-0.201 |
0.000 |
| y |
-0.201 |
1.525 |
0.000 |
| z |
0.000 |
0.000 |
3.988 |
<r2> (average value of r
2) Å
2
| <r2> |
105.032 |
| (<r2>)1/2 |
10.249 |