Jump to
S1C2
Energy calculated at B3PW91/aug-cc-pVTZ
| hartrees |
Energy at 0K | -759.473525 |
Energy at 298.15K | |
HF Energy | -759.473525 |
Nuclear repulsion energy | 182.374329 |
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/aug-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' |
568 |
548 |
0.00 |
|
|
|
2 |
A2" |
427 |
412 |
22.06 |
|
|
|
3 |
E' |
113i |
109i |
2.88 |
|
|
|
3 |
E' |
113i |
109i |
2.88 |
|
|
|
4 |
E' |
578 |
558 |
292.78 |
|
|
|
4 |
E' |
578 |
558 |
292.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 962.4 cm
-1
Scaled (by 0.9651) Zero Point Vibrational Energy (zpe) 928.8 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/aug-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 |
1.739 |
0.000 |
F3 |
1.506 |
-0.869 |
0.000 |
F4 |
-1.506 |
-0.869 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7389 | 1.7389 | 1.7389 |
F2 | 1.7389 | | 3.0119 | 3.0119 | F3 | 1.7389 | 3.0119 | | 3.0119 | F4 | 1.7389 | 3.0119 | 3.0119 | |
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
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.128 |
|
|
|
2 |
F |
-0.376 |
|
|
|
3 |
F |
-0.376 |
|
|
|
4 |
F |
-0.376 |
|
|
|
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 |
-29.872 |
0.000 |
0.000 |
y |
0.000 |
-29.872 |
0.000 |
z |
0.000 |
0.000 |
-26.566 |
|
Traceless |
| x | y | z |
x |
-1.653 |
0.000 |
0.000 |
y |
0.000 |
-1.653 |
0.000 |
z |
0.000 |
0.000 |
3.306 |
|
Polar |
3z2-r2 | 6.612 |
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 |
5.799 |
0.000 |
0.000 |
y |
0.000 |
5.799 |
0.000 |
z |
0.000 |
0.000 |
2.704 |
<r2> (average value of r
2) Å
2
<r2> |
99.613 |
(<r2>)1/2 |
9.981 |
Jump to
S1C1
Energy calculated at B3PW91/aug-cc-pVTZ
| hartrees |
Energy at 0K | -759.503775 |
Energy at 298.15K | -759.505124 |
HF Energy | -759.503775 |
Nuclear repulsion energy | 194.099220 |
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/aug-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 |
770 |
743 |
50.02 |
|
|
|
2 |
A1 |
538 |
519 |
4.18 |
|
|
|
3 |
A1 |
314 |
303 |
12.21 |
|
|
|
4 |
B1 |
330 |
319 |
15.95 |
|
|
|
5 |
B2 |
708 |
683 |
508.10 |
|
|
|
6 |
B2 |
421 |
406 |
0.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1540.3 cm
-1
Scaled (by 0.9651) Zero Point Vibrational Energy (zpe) 1486.5 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/aug-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 |
-1.255 |
F3 |
0.000 |
1.716 |
0.289 |
F4 |
0.000 |
-1.716 |
0.289 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.6133 | 1.7174 | 1.7174 |
F2 | 1.6133 | | 2.3084 | 2.3084 | F3 | 1.7174 | 2.3084 | | 3.4320 | F4 | 1.7174 | 2.3084 | 3.4320 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.692 |
|
F2 |
Cl1 |
F4 |
87.692 |
F3 |
Cl1 |
F4 |
175.384 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.105 |
|
|
|
2 |
F |
-0.282 |
|
|
|
3 |
F |
-0.411 |
|
|
|
4 |
F |
-0.411 |
|
|
|
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 |
0.605 |
0.605 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.319 |
0.000 |
0.000 |
y |
0.000 |
-32.979 |
0.000 |
z |
0.000 |
0.000 |
-25.572 |
|
Traceless |
| x | y | z |
x |
2.957 |
0.000 |
0.000 |
y |
0.000 |
-7.033 |
0.000 |
z |
0.000 |
0.000 |
4.077 |
|
Polar |
3z2-r2 | 8.153 |
x2-y2 | 6.660 |
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 |
2.660 |
0.000 |
0.000 |
y |
0.000 |
6.036 |
0.000 |
z |
0.000 |
0.000 |
3.709 |
<r2> (average value of r
2) Å
2
<r2> |
88.535 |
(<r2>)1/2 |
9.409 |