Jump to
S1C2
Energy calculated at B3PW91/cc-pVDZ
| hartrees |
Energy at 0K | -759.319349 |
Energy at 298.15K | |
HF Energy | -759.319349 |
Nuclear repulsion energy | 179.410706 |
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/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' |
553 |
533 |
0.00 |
|
|
|
2 |
A2" |
406 |
391 |
29.93 |
|
|
|
3 |
E' |
74i |
71i |
0.23 |
|
|
|
3 |
E' |
74i |
71i |
0.23 |
|
|
|
4 |
E' |
602 |
581 |
208.89 |
|
|
|
4 |
E' |
602 |
581 |
208.88 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1007.1 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 971.9 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 B3PW91/cc-pVDZ
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.000 |
F2 |
0.000 |
1.768 |
0.000 |
F3 |
1.531 |
-0.884 |
0.000 |
F4 |
-1.531 |
-0.884 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7676 | 1.7676 | 1.7676 |
F2 | 1.7676 | | 3.0616 | 3.0616 | F3 | 1.7676 | 3.0616 | | 3.0616 | F4 | 1.7676 | 3.0616 | 3.0616 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
120.000 |
|
F2 |
Cl1 |
F4 |
120.000 |
F3 |
Cl1 |
F4 |
120.000 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.909 |
|
|
|
2 |
F |
-0.303 |
|
|
|
3 |
F |
-0.303 |
|
|
|
4 |
F |
-0.303 |
|
|
|
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 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-29.588 |
0.000 |
0.000 |
y |
0.000 |
-29.588 |
0.000 |
z |
0.000 |
0.000 |
-25.849 |
|
Traceless |
| x | y | z |
x |
-1.869 |
0.000 |
0.000 |
y |
0.000 |
-1.869 |
0.000 |
z |
0.000 |
0.000 |
3.739 |
|
Polar |
3z2-r2 | 7.478 |
x2-y2 | 0.000 |
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 |
4.534 |
0.000 |
0.000 |
y |
0.000 |
4.534 |
0.000 |
z |
0.000 |
0.000 |
1.093 |
<r2> (average value of r
2) Å
2
<r2> |
102.065 |
(<r2>)1/2 |
10.103 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVDZ
| hartrees |
Energy at 0K | -759.343771 |
Energy at 298.15K | -759.345044 |
HF Energy | -759.343771 |
Nuclear repulsion energy | 190.849364 |
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/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 |
728 |
703 |
41.15 |
|
|
|
2 |
A1 |
534 |
516 |
3.34 |
|
|
|
3 |
A1 |
296 |
285 |
14.33 |
|
|
|
4 |
B1 |
316 |
305 |
20.80 |
|
|
|
5 |
B2 |
748 |
722 |
383.31 |
|
|
|
6 |
B2 |
391 |
377 |
1.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1506.2 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 1453.5 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/cc-pVDZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.370 |
F2 |
0.000 |
0.000 |
-1.286 |
F3 |
0.000 |
1.737 |
0.294 |
F4 |
0.000 |
-1.737 |
0.294 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.6565 | 1.7388 | 1.7388 |
F2 | 1.6565 | | 2.3482 | 2.3482 | F3 | 1.7388 | 2.3482 | | 3.4742 | F4 | 1.7388 | 2.3482 | 3.4742 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.479 |
|
F2 |
Cl1 |
F4 |
87.479 |
F3 |
Cl1 |
F4 |
174.957 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.913 |
|
|
|
2 |
F |
-0.203 |
|
|
|
3 |
F |
-0.355 |
|
|
|
4 |
F |
-0.355 |
|
|
|
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 |
0.943 |
0.943 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.629 |
0.000 |
0.000 |
y |
0.000 |
-32.775 |
0.000 |
z |
0.000 |
0.000 |
-25.056 |
|
Traceless |
| x | y | z |
x |
3.286 |
0.000 |
0.000 |
y |
0.000 |
-7.432 |
0.000 |
z |
0.000 |
0.000 |
4.146 |
|
Polar |
3z2-r2 | 8.293 |
x2-y2 | 7.146 |
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 |
1.153 |
0.000 |
0.000 |
y |
0.000 |
4.882 |
0.000 |
z |
0.000 |
0.000 |
2.577 |
<r2> (average value of r
2) Å
2
<r2> |
90.465 |
(<r2>)1/2 |
9.511 |