Jump to
S1C2
Energy calculated at B3PW91/6-31+G**
| hartrees |
Energy at 0K | -759.316178 |
Energy at 298.15K | |
HF Energy | -759.316178 |
Nuclear repulsion energy | 180.330886 |
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 B3PW91/6-31+G**
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' |
554 |
532 |
0.00 |
|
|
|
2 |
A2" |
411 |
394 |
28.06 |
|
|
|
3 |
E' |
89i |
86i |
1.46 |
|
|
|
3 |
E' |
89i |
86i |
1.46 |
|
|
|
4 |
E' |
578 |
555 |
285.31 |
|
|
|
4 |
E' |
578 |
555 |
285.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 971.0 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 932.2 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 B3PW91/6-31+G**
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.000 |
F2 |
0.000 |
1.759 |
0.000 |
F3 |
1.523 |
-0.879 |
0.000 |
F4 |
-1.523 |
-0.879 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7586 | 1.7586 | 1.7586 |
F2 | 1.7586 | | 3.0460 | 3.0460 | F3 | 1.7586 | 3.0460 | | 3.0460 | F4 | 1.7586 | 3.0460 | 3.0460 | |
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 B3PW91/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.899 |
|
|
|
2 |
F |
-0.300 |
|
|
|
3 |
F |
-0.300 |
|
|
|
4 |
F |
-0.300 |
|
|
|
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 |
-30.561 |
0.000 |
0.000 |
y |
0.000 |
-30.561 |
0.000 |
z |
0.000 |
0.000 |
-26.647 |
|
Traceless |
| x | y | z |
x |
-1.957 |
0.000 |
0.000 |
y |
0.000 |
-1.957 |
0.000 |
z |
0.000 |
0.000 |
3.914 |
|
Polar |
3z2-r2 | 7.828 |
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 |
5.608 |
0.000 |
0.000 |
y |
0.000 |
5.607 |
0.000 |
z |
0.000 |
0.000 |
2.030 |
<r2> (average value of r
2) Å
2
<r2> |
101.777 |
(<r2>)1/2 |
10.088 |
Jump to
S1C1
Energy calculated at B3PW91/6-31+G**
| hartrees |
Energy at 0K | -759.341751 |
Energy at 298.15K | -759.343014 |
HF Energy | -759.341751 |
Nuclear repulsion energy | 191.728834 |
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 B3PW91/6-31+G**
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 |
747 |
717 |
49.70 |
|
|
|
2 |
A1 |
526 |
505 |
4.03 |
|
|
|
3 |
A1 |
298 |
286 |
15.70 |
|
|
|
4 |
B1 |
317 |
304 |
22.14 |
|
|
|
5 |
B2 |
711 |
683 |
493.76 |
|
|
|
6 |
B2 |
399 |
384 |
0.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1498.6 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 1438.8 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 B3PW91/6-31+G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.366 |
F2 |
0.000 |
0.000 |
-1.274 |
F3 |
0.000 |
1.734 |
0.291 |
F4 |
0.000 |
-1.734 |
0.291 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.6407 | 1.7352 | 1.7352 |
F2 | 1.6407 | | 2.3361 | 2.3361 | F3 | 1.7352 | 2.3361 | | 3.4671 | F4 | 1.7352 | 2.3361 | 3.4671 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.530 |
|
F2 |
Cl1 |
F4 |
87.530 |
F3 |
Cl1 |
F4 |
175.060 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.044 |
|
|
|
2 |
F |
-0.242 |
|
|
|
3 |
F |
-0.401 |
|
|
|
4 |
F |
-0.401 |
|
|
|
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 |
0.861 |
0.861 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.378 |
0.000 |
0.000 |
y |
0.000 |
-34.029 |
0.000 |
z |
0.000 |
0.000 |
-25.741 |
|
Traceless |
| x | y | z |
x |
3.507 |
0.000 |
0.000 |
y |
0.000 |
-7.970 |
0.000 |
z |
0.000 |
0.000 |
4.463 |
|
Polar |
3z2-r2 | 8.926 |
x2-y2 | 7.651 |
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 |
2.109 |
0.000 |
0.000 |
y |
0.000 |
5.936 |
0.000 |
z |
0.000 |
0.000 |
3.273 |
<r2> (average value of r
2) Å
2
<r2> |
90.457 |
(<r2>)1/2 |
9.511 |