Jump to
S1C2
Energy calculated at B3LYP/SDD
| | hartrees |
| Energy at 0K | -958.976300 |
| Energy at 298.15K | |
| HF Energy | -958.976300 |
| Nuclear repulsion energy | 120.468761 |
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 B3LYP/SDD
| 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 |
3310 |
3182 |
0.66 |
|
|
|
| 2 |
A1 |
672 |
646 |
14.66 |
|
|
|
| 3 |
A1 |
285 |
274 |
0.40 |
|
|
|
| 4 |
B1 |
410i |
395i |
115.20 |
|
|
|
| 5 |
B2 |
1206 |
1160 |
42.02 |
|
|
|
| 6 |
B2 |
838 |
806 |
168.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2950.1 cm
-1
Scaled (by 0.9613) Zero Point Vibrational Energy (zpe) 2835.9 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 B3LYP/SDD
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.705 |
| H2 |
0.000 |
0.000 |
1.785 |
| Cl3 |
0.000 |
1.543 |
-0.177 |
| Cl4 |
0.000 |
-1.543 |
-0.177 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0800 | 1.7768 | 1.7768 |
H2 | 1.0800 | | 2.4955 | 2.4955 | Cl3 | 1.7768 | 2.4955 | | 3.0856 | Cl4 | 1.7768 | 2.4955 | 3.0856 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.740 |
|
Cl3 |
C1 |
Cl4 |
120.519 |
| Cl4 |
C1 |
H2 |
119.740 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/SDD
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.397 |
|
|
|
| 2 |
H |
0.291 |
|
|
|
| 3 |
Cl |
0.053 |
|
|
|
| 4 |
Cl |
0.053 |
|
|
|
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 |
1.190 |
1.190 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.127 |
0.000 |
0.000 |
| y |
0.000 |
-31.991 |
0.000 |
| z |
0.000 |
0.000 |
-28.757 |
|
| Traceless |
| | x | y | z |
| x |
-1.753 |
0.000 |
0.000 |
| y |
0.000 |
-1.548 |
0.000 |
| z |
0.000 |
0.000 |
3.302 |
|
| Polar |
| 3z2-r2 | 6.603 |
| x2-y2 | -0.137 |
| 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 |
1.450 |
0.000 |
0.000 |
| y |
0.000 |
6.440 |
0.000 |
| z |
0.000 |
0.000 |
2.990 |
<r2> (average value of r
2) Å
2
| <r2> |
107.489 |
| (<r2>)1/2 |
10.368 |
Jump to
S1C1
Energy calculated at B3LYP/SDD
| | hartrees |
| Energy at 0K | -958.977726 |
| Energy at 298.15K | -958.978443 |
| HF Energy | -958.977726 |
| Nuclear repulsion energy | 120.089989 |
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 B3LYP/SDD
| 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' |
3253 |
3127 |
3.92 |
|
|
|
| 2 |
A' |
696 |
669 |
30.22 |
|
|
|
| 3 |
A' |
513 |
493 |
26.34 |
|
|
|
| 4 |
A' |
279 |
268 |
0.47 |
|
|
|
| 5 |
A" |
1219 |
1172 |
33.28 |
|
|
|
| 6 |
A" |
794 |
763 |
193.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3377.0 cm
-1
Scaled (by 0.9613) Zero Point Vibrational Energy (zpe) 3246.3 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 B3LYP/SDD
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.014 |
0.739 |
0.000 |
| H2 |
-0.562 |
1.659 |
0.000 |
| Cl3 |
0.014 |
-0.179 |
1.540 |
| Cl4 |
0.014 |
-0.179 |
-1.540 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0851 | 1.7929 | 1.7929 |
H2 | 1.0851 | | 2.4658 | 2.4658 | Cl3 | 1.7929 | 2.4658 | | 3.0799 | Cl4 | 1.7929 | 2.4658 | 3.0799 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
115.721 |
|
Cl3 |
C1 |
Cl4 |
118.393 |
| Cl4 |
C1 |
H2 |
115.721 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/SDD
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.350 |
|
|
|
| 2 |
H |
0.276 |
|
|
|
| 3 |
Cl |
0.037 |
|
|
|
| 4 |
Cl |
0.037 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.798 |
1.073 |
0.000 |
1.337 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.690 |
-1.219 |
0.000 |
| y |
-1.219 |
-29.403 |
0.000 |
| z |
0.000 |
0.000 |
-32.331 |
|
| Traceless |
| | x | y | z |
| x |
-0.823 |
-1.219 |
0.000 |
| y |
-1.219 |
2.607 |
0.000 |
| z |
0.000 |
0.000 |
-1.785 |
|
| Polar |
| 3z2-r2 | -3.570 |
| x2-y2 | -2.287 |
| xy | -1.219 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.541 |
-0.169 |
0.000 |
| y |
-0.169 |
3.089 |
0.000 |
| z |
0.000 |
0.000 |
6.563 |
<r2> (average value of r
2) Å
2
| <r2> |
107.521 |
| (<r2>)1/2 |
10.369 |