Jump to
S1C2
Energy calculated at PBE1PBE/aug-cc-pVDZ
| hartrees |
Energy at 0K | -958.712609 |
Energy at 298.15K | |
HF Energy | -958.712609 |
Nuclear repulsion energy | 125.790341 |
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/aug-cc-pVDZ
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 |
3284 |
3158 |
0.99 |
|
|
|
2 |
A1 |
772 |
742 |
6.84 |
|
|
|
3 |
A1 |
312 |
300 |
0.38 |
|
|
|
4 |
B1 |
364i |
350i |
35.63 |
|
|
|
5 |
B2 |
1217 |
1171 |
53.48 |
|
|
|
6 |
B2 |
947 |
910 |
139.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3083.8 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 2965.4 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/aug-cc-pVDZ
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 |
1.760 |
Cl3 |
0.000 |
1.473 |
-0.171 |
Cl4 |
0.000 |
-1.473 |
-0.171 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0852 | 1.6987 | 1.6987 |
H2 | 1.0852 | | 2.4289 | 2.4289 | Cl3 | 1.6987 | 2.4289 | | 2.9462 | Cl4 | 1.6987 | 2.4289 | 2.9462 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.866 |
|
Cl3 |
C1 |
Cl4 |
120.268 |
Cl4 |
C1 |
H2 |
119.866 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.002 |
|
|
|
2 |
H |
-0.077 |
|
|
|
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 |
|
0.000 |
0.000 |
0.953 |
0.953 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.162 |
0.000 |
0.000 |
y |
0.000 |
-31.016 |
0.000 |
z |
0.000 |
0.000 |
-28.999 |
|
Traceless |
| x | y | z |
x |
-2.154 |
0.000 |
0.000 |
y |
0.000 |
-0.435 |
0.000 |
z |
0.000 |
0.000 |
2.590 |
|
Polar |
3z2-r2 | 5.179 |
x2-y2 | -1.146 |
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 |
4.538 |
0.000 |
0.000 |
y |
0.000 |
8.094 |
0.000 |
z |
0.000 |
0.000 |
5.377 |
<r2> (average value of r
2) Å
2
<r2> |
99.798 |
(<r2>)1/2 |
9.990 |
Jump to
S1C1
Energy calculated at PBE1PBE/aug-cc-pVDZ
| hartrees |
Energy at 0K | -958.713442 |
Energy at 298.15K | -958.714251 |
HF Energy | -958.713442 |
Nuclear repulsion energy | 125.649859 |
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/aug-cc-pVDZ
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' |
3239 |
3114 |
0.66 |
|
|
|
2 |
A' |
776 |
746 |
11.41 |
|
|
|
3 |
A' |
484 |
466 |
21.94 |
|
|
|
4 |
A' |
305 |
293 |
0.58 |
|
|
|
5 |
A" |
1219 |
1172 |
41.65 |
|
|
|
6 |
A" |
914 |
879 |
166.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3468.1 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 3334.9 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 PBE1PBE/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
0.700 |
0.000 |
H2 |
-0.497 |
1.662 |
0.000 |
Cl3 |
0.012 |
-0.172 |
1.469 |
Cl4 |
0.012 |
-0.172 |
-1.469 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0888 | 1.7083 | 1.7083 |
H2 | 1.0888 | | 2.4047 | 2.4047 | Cl3 | 1.7083 | 2.4047 | | 2.9377 | Cl4 | 1.7083 | 2.4047 | 2.9377 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
116.831 |
|
Cl3 |
C1 |
Cl4 |
118.597 |
Cl4 |
C1 |
H2 |
116.831 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.077 |
|
|
|
2 |
H |
-0.016 |
|
|
|
3 |
Cl |
0.047 |
|
|
|
4 |
Cl |
0.047 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.450 |
0.861 |
0.000 |
0.972 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.856 |
-0.935 |
0.000 |
y |
-0.935 |
-29.445 |
0.000 |
z |
0.000 |
0.000 |
-31.120 |
|
Traceless |
| x | y | z |
x |
-1.574 |
-0.935 |
0.000 |
y |
-0.935 |
2.043 |
0.000 |
z |
0.000 |
0.000 |
-0.469 |
|
Polar |
3z2-r2 | -0.938 |
x2-y2 | -2.411 |
xy | -0.935 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.582 |
-0.065 |
0.000 |
y |
-0.065 |
5.411 |
0.000 |
z |
0.000 |
0.000 |
8.181 |
<r2> (average value of r
2) Å
2
<r2> |
99.562 |
(<r2>)1/2 |
9.978 |