Jump to
S1C2
Energy calculated at HF/cc-pVDZ
| hartrees |
Energy at 0K | -757.440891 |
Energy at 298.15K | |
HF Energy | -757.440891 |
Nuclear repulsion energy | 185.109434 |
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 HF/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' |
632 |
574 |
0.00 |
|
|
|
2 |
A2" |
485 |
440 |
60.47 |
|
|
|
3 |
E' |
236i |
215i |
31.52 |
|
|
|
3 |
E' |
236i |
215i |
31.52 |
|
|
|
4 |
E' |
633 |
575 |
461.51 |
|
|
|
4 |
E' |
633 |
575 |
461.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 955.6 cm
-1
Scaled (by 0.908) Zero Point Vibrational Energy (zpe) 867.7 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 HF/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 |
1.713 |
0.000 |
F3 |
1.484 |
-0.857 |
0.000 |
F4 |
-1.484 |
-0.857 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7132 | 1.7132 | 1.7132 |
F2 | 1.7132 | | 2.9674 | 2.9674 | F3 | 1.7132 | 2.9674 | | 2.9674 | F4 | 1.7132 | 2.9674 | 2.9674 | |
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 HF/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.288 |
|
|
|
2 |
F |
-0.429 |
|
|
|
3 |
F |
-0.429 |
|
|
|
4 |
F |
-0.429 |
|
|
|
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 |
-31.409 |
0.000 |
0.000 |
y |
0.000 |
-31.409 |
0.000 |
z |
0.000 |
0.000 |
-25.779 |
|
Traceless |
| x | y | z |
x |
-2.815 |
0.000 |
0.000 |
y |
0.000 |
-2.815 |
0.000 |
z |
0.000 |
0.000 |
5.630 |
|
Polar |
3z2-r2 | 11.260 |
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 |
4.675 |
0.000 |
0.000 |
y |
0.000 |
4.675 |
0.000 |
z |
0.000 |
0.000 |
1.023 |
<r2> (average value of r
2) Å
2
<r2> |
97.694 |
(<r2>)1/2 |
9.884 |
Jump to
S1C1
Energy calculated at HF/cc-pVDZ
| hartrees |
Energy at 0K | -757.509326 |
Energy at 298.15K | -757.510955 |
HF Energy | -757.509326 |
Nuclear repulsion energy | 197.466236 |
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 HF/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 |
891 |
809 |
42.15 |
|
|
|
2 |
A1 |
622 |
565 |
0.92 |
|
|
|
3 |
A1 |
384 |
348 |
26.97 |
|
|
|
4 |
B1 |
368 |
335 |
33.16 |
|
|
|
5 |
B2 |
770 |
699 |
674.64 |
|
|
|
6 |
B2 |
483 |
438 |
1.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1759.0 cm
-1
Scaled (by 0.908) Zero Point Vibrational Energy (zpe) 1597.1 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 HF/cc-pVDZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.369 |
F2 |
0.000 |
0.000 |
-1.222 |
F3 |
0.000 |
1.688 |
0.263 |
F4 |
0.000 |
-1.688 |
0.263 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.5913 | 1.6911 | 1.6911 |
F2 | 1.5913 | | 2.2479 | 2.2479 | F3 | 1.6911 | 2.2479 | | 3.3755 | F4 | 1.6911 | 2.2479 | 3.3755 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
86.387 |
|
F2 |
Cl1 |
F4 |
86.387 |
F3 |
Cl1 |
F4 |
172.775 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.176 |
|
|
|
2 |
F |
-0.236 |
|
|
|
3 |
F |
-0.470 |
|
|
|
4 |
F |
-0.470 |
|
|
|
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 |
1.012 |
1.012 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.582 |
0.000 |
0.000 |
y |
0.000 |
-34.933 |
0.000 |
z |
0.000 |
0.000 |
-25.099 |
|
Traceless |
| x | y | z |
x |
4.434 |
0.000 |
0.000 |
y |
0.000 |
-9.593 |
0.000 |
z |
0.000 |
0.000 |
5.159 |
|
Polar |
3z2-r2 | 10.318 |
x2-y2 | 9.351 |
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 |
1.122 |
0.000 |
0.000 |
y |
0.000 |
4.509 |
0.000 |
z |
0.000 |
0.000 |
2.386 |
<r2> (average value of r
2) Å
2
<r2> |
86.098 |
(<r2>)1/2 |
9.279 |