Jump to
S1C2
Energy calculated at B3PW91/cc-pVTZ
| hartrees |
Energy at 0K | -759.461989 |
Energy at 298.15K | |
HF Energy | -759.461989 |
Nuclear repulsion energy | 182.530983 |
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-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' |
570 |
548 |
0.00 |
|
|
|
2 |
A2" |
431 |
414 |
25.67 |
|
|
|
3 |
E' |
112i |
108i |
1.86 |
|
|
|
3 |
E' |
112i |
108i |
1.86 |
|
|
|
4 |
E' |
589 |
566 |
280.39 |
|
|
|
4 |
E' |
589 |
566 |
280.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 976.6 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 939.1 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-pVTZ
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.000 |
F2 |
0.000 |
1.737 |
0.000 |
F3 |
1.505 |
-0.869 |
0.000 |
F4 |
-1.505 |
-0.869 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7374 | 1.7374 | 1.7374 |
F2 | 1.7374 | | 3.0093 | 3.0093 | F3 | 1.7374 | 3.0093 | | 3.0093 | F4 | 1.7374 | 3.0093 | 3.0093 | |
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-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.826 |
|
|
|
2 |
F |
-0.275 |
|
|
|
3 |
F |
-0.275 |
|
|
|
4 |
F |
-0.275 |
|
|
|
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 |
-29.468 |
0.000 |
0.000 |
y |
0.000 |
-29.468 |
0.000 |
z |
0.000 |
0.000 |
-26.190 |
|
Traceless |
| x | y | z |
x |
-1.639 |
0.000 |
0.000 |
y |
0.000 |
-1.639 |
0.000 |
z |
0.000 |
0.000 |
3.278 |
|
Polar |
3z2-r2 | 6.557 |
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 |
4.894 |
0.000 |
0.000 |
y |
0.000 |
4.893 |
0.000 |
z |
0.000 |
0.000 |
1.708 |
<r2> (average value of r
2) Å
2
<r2> |
99.226 |
(<r2>)1/2 |
9.961 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVTZ
| hartrees |
Energy at 0K | -759.492181 |
Energy at 298.15K | -759.493549 |
HF Energy | -759.492181 |
Nuclear repulsion energy | 194.341949 |
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-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 |
768 |
738 |
53.44 |
|
|
|
2 |
A1 |
542 |
521 |
4.16 |
|
|
|
3 |
A1 |
317 |
304 |
12.89 |
|
|
|
4 |
B1 |
334 |
321 |
17.32 |
|
|
|
5 |
B2 |
726 |
698 |
483.54 |
|
|
|
6 |
B2 |
424 |
407 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1554.6 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 1494.9 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-pVTZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.358 |
F2 |
0.000 |
0.000 |
-1.256 |
F3 |
0.000 |
1.712 |
0.290 |
F4 |
0.000 |
-1.712 |
0.290 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.6142 | 1.7135 | 1.7135 |
F2 | 1.6142 | | 2.3068 | 2.3068 | F3 | 1.7135 | 2.3068 | | 3.4242 | F4 | 1.7135 | 2.3068 | 3.4242 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.716 |
|
F2 |
Cl1 |
F4 |
87.716 |
F3 |
Cl1 |
F4 |
175.432 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.776 |
|
|
|
2 |
F |
-0.142 |
|
|
|
3 |
F |
-0.317 |
|
|
|
4 |
F |
-0.317 |
|
|
|
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 |
0.664 |
0.664 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.959 |
0.000 |
0.000 |
y |
0.000 |
-32.516 |
0.000 |
z |
0.000 |
0.000 |
-25.194 |
|
Traceless |
| x | y | z |
x |
2.896 |
0.000 |
0.000 |
y |
0.000 |
-6.940 |
0.000 |
z |
0.000 |
0.000 |
4.043 |
|
Polar |
3z2-r2 | 8.087 |
x2-y2 | 6.557 |
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 |
1.743 |
0.000 |
0.000 |
y |
0.000 |
5.169 |
0.000 |
z |
0.000 |
0.000 |
2.931 |
<r2> (average value of r
2) Å
2
<r2> |
88.075 |
(<r2>)1/2 |
9.385 |