Jump to
S1C2
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -958.750214 |
| Energy at 298.15K | |
| HF Energy | -958.750214 |
| Nuclear repulsion energy | 126.442383 |
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 PBE1PBE/cc-pVTZ
| 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 |
3273 |
3146 |
0.20 |
|
|
|
| 2 |
A1 |
770 |
740 |
8.23 |
|
|
|
| 3 |
A1 |
312 |
300 |
0.38 |
|
|
|
| 4 |
B1 |
321i |
308i |
40.28 |
|
|
|
| 5 |
B2 |
1233 |
1184 |
49.24 |
|
|
|
| 6 |
B2 |
944 |
907 |
144.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3105.5 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 2984.4 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 PBE1PBE/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.667 |
| H2 |
0.000 |
0.000 |
1.744 |
| Cl3 |
0.000 |
1.467 |
-0.169 |
| Cl4 |
0.000 |
-1.467 |
-0.169 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0763 | 1.6889 | 1.6889 |
H2 | 1.0763 | | 2.4106 | 2.4106 | Cl3 | 1.6889 | 2.4106 | | 2.9347 | Cl4 | 1.6889 | 2.4106 | 2.9347 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.680 |
|
Cl3 |
C1 |
Cl4 |
120.639 |
| Cl4 |
C1 |
H2 |
119.680 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.098 |
|
|
|
| 2 |
H |
0.157 |
|
|
|
| 3 |
Cl |
-0.029 |
|
|
|
| 4 |
Cl |
-0.029 |
|
|
|
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 |
0.906 |
0.906 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.693 |
0.000 |
0.000 |
| y |
0.000 |
-30.781 |
0.000 |
| z |
0.000 |
0.000 |
-28.792 |
|
| Traceless |
| | x | y | z |
| x |
-1.907 |
0.000 |
0.000 |
| y |
0.000 |
-0.539 |
0.000 |
| z |
0.000 |
0.000 |
2.446 |
|
| Polar |
| 3z2-r2 | 4.892 |
| x2-y2 | -0.912 |
| 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 |
3.295 |
0.000 |
0.000 |
| y |
0.000 |
7.329 |
0.000 |
| z |
0.000 |
0.000 |
4.402 |
<r2> (average value of r
2) Å
2
| <r2> |
98.890 |
| (<r2>)1/2 |
9.944 |
Jump to
S1C1
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -958.750697 |
| Energy at 298.15K | -958.751461 |
| HF Energy | -958.750697 |
| Nuclear repulsion energy | 126.317808 |
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 PBE1PBE/cc-pVTZ
| 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' |
3241 |
3115 |
0.72 |
|
|
|
| 2 |
A' |
774 |
744 |
11.95 |
|
|
|
| 3 |
A' |
432 |
415 |
26.04 |
|
|
|
| 4 |
A' |
304 |
292 |
1.26 |
|
|
|
| 5 |
A" |
1236 |
1188 |
41.27 |
|
|
|
| 6 |
A" |
919 |
883 |
163.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3452.9 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 3318.3 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 PBE1PBE/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.686 |
0.000 |
| H2 |
-0.431 |
1.671 |
0.000 |
| Cl3 |
0.011 |
-0.170 |
1.464 |
| Cl4 |
0.011 |
-0.170 |
-1.464 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0790 | 1.6964 | 1.6964 |
H2 | 1.0790 | | 2.3935 | 2.3935 | Cl3 | 1.6964 | 2.3935 | | 2.9284 | Cl4 | 1.6964 | 2.3935 | 2.9284 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.433 |
|
Cl3 |
C1 |
Cl4 |
119.335 |
| Cl4 |
C1 |
H2 |
117.433 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.089 |
|
|
|
| 2 |
H |
0.152 |
|
|
|
| 3 |
Cl |
-0.032 |
|
|
|
| 4 |
Cl |
-0.032 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.410 |
0.836 |
0.000 |
0.931 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.476 |
-0.798 |
0.000 |
| y |
-0.798 |
-29.124 |
0.000 |
| z |
0.000 |
0.000 |
-30.865 |
|
| Traceless |
| | x | y | z |
| x |
-1.481 |
-0.798 |
0.000 |
| y |
-0.798 |
2.046 |
0.000 |
| z |
0.000 |
0.000 |
-0.565 |
|
| Polar |
| 3z2-r2 | -1.130 |
| x2-y2 | -2.352 |
| xy | -0.798 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.350 |
-0.114 |
0.000 |
| y |
-0.114 |
4.429 |
0.000 |
| z |
0.000 |
0.000 |
7.375 |
<r2> (average value of r
2) Å
2
| <r2> |
98.731 |
| (<r2>)1/2 |
9.936 |