Jump to
S1C2
Energy calculated at PBEPBE/TZVP
| | hartrees |
| Energy at 0K | -958.645855 |
| Energy at 298.15K | |
| HF Energy | -958.645855 |
| Nuclear repulsion energy | 124.648257 |
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 PBEPBE/TZVP
| 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 |
3196 |
3160 |
0.03 |
|
|
|
| 2 |
A1 |
733 |
725 |
8.33 |
|
|
|
| 3 |
A1 |
303 |
300 |
0.15 |
|
|
|
| 4 |
B1 |
336i |
333i |
62.62 |
|
|
|
| 5 |
B2 |
1202 |
1188 |
41.56 |
|
|
|
| 6 |
B2 |
885 |
875 |
176.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2991.4 cm
-1
Scaled (by 0.9888) Zero Point Vibrational Energy (zpe) 2957.9 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 PBEPBE/TZVP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.672 |
| H2 |
0.000 |
0.000 |
1.757 |
| Cl3 |
0.000 |
1.491 |
-0.170 |
| Cl4 |
0.000 |
-1.491 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0844 | 1.7124 | 1.7124 |
H2 | 1.0844 | | 2.4364 | 2.4364 | Cl3 | 1.7124 | 2.4364 | | 2.9814 | Cl4 | 1.7124 | 2.4364 | 2.9814 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.480 |
|
Cl3 |
C1 |
Cl4 |
121.040 |
| Cl4 |
C1 |
H2 |
119.480 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.245 |
|
|
|
| 2 |
H |
0.213 |
|
|
|
| 3 |
Cl |
0.016 |
|
|
|
| 4 |
Cl |
0.016 |
|
|
|
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 |
0.825 |
0.825 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.064 |
0.000 |
0.000 |
| y |
0.000 |
-30.789 |
0.000 |
| z |
0.000 |
0.000 |
-29.045 |
|
| Traceless |
| | x | y | z |
| x |
-2.147 |
0.000 |
0.000 |
| y |
0.000 |
-0.234 |
0.000 |
| z |
0.000 |
0.000 |
2.381 |
|
| Polar |
| 3z2-r2 | 4.763 |
| x2-y2 | -1.275 |
| 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 |
2.897 |
0.000 |
0.000 |
| y |
0.000 |
7.286 |
0.000 |
| z |
0.000 |
0.000 |
4.060 |
<r2> (average value of r
2) Å
2
| <r2> |
101.473 |
| (<r2>)1/2 |
10.073 |
Jump to
S1C1
Energy calculated at PBEPBE/TZVP
| | hartrees |
| Energy at 0K | -958.646545 |
| Energy at 298.15K | -958.647276 |
| HF Energy | -958.646545 |
| Nuclear repulsion energy | 124.454555 |
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 PBEPBE/TZVP
| 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' |
3155 |
3120 |
1.41 |
|
|
|
| 2 |
A' |
738 |
730 |
13.78 |
|
|
|
| 3 |
A' |
445 |
440 |
31.87 |
|
|
|
| 4 |
A' |
297 |
293 |
0.84 |
|
|
|
| 5 |
A" |
1204 |
1191 |
35.02 |
|
|
|
| 6 |
A" |
852 |
842 |
199.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3345.2 cm
-1
Scaled (by 0.9888) Zero Point Vibrational Energy (zpe) 3307.7 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 PBEPBE/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.696 |
0.000 |
| H2 |
-0.480 |
1.666 |
0.000 |
| Cl3 |
0.012 |
-0.172 |
1.488 |
| Cl4 |
0.012 |
-0.172 |
-1.488 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0877 | 1.7222 | 1.7222 |
H2 | 1.0877 | | 2.4151 | 2.4151 | Cl3 | 1.7222 | 2.4151 | | 2.9752 | Cl4 | 1.7222 | 2.4151 | 2.9752 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.709 |
|
Cl3 |
C1 |
Cl4 |
119.486 |
| Cl4 |
C1 |
H2 |
116.709 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.210 |
|
|
|
| 2 |
H |
0.195 |
|
|
|
| 3 |
Cl |
0.007 |
|
|
|
| 4 |
Cl |
0.007 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.531 |
0.738 |
0.000 |
0.909 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.775 |
-0.963 |
0.000 |
| y |
-0.963 |
-29.489 |
0.000 |
| z |
0.000 |
0.000 |
-30.953 |
|
| Traceless |
| | x | y | z |
| x |
-1.554 |
-0.963 |
0.000 |
| y |
-0.963 |
1.875 |
0.000 |
| z |
0.000 |
0.000 |
-0.321 |
|
| Polar |
| 3z2-r2 | -0.642 |
| x2-y2 | -2.286 |
| xy | -0.963 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.969 |
-0.108 |
0.000 |
| y |
-0.108 |
4.123 |
0.000 |
| z |
0.000 |
0.000 |
7.355 |
<r2> (average value of r
2) Å
2
| <r2> |
101.360 |
| (<r2>)1/2 |
10.068 |