Jump to
S1C2
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -695.893424 |
| Energy at 298.15K | -695.894883 |
| HF Energy | -695.893424 |
| Nuclear repulsion energy | 196.731055 |
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/Def2TZVPP
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
984 |
892 |
144.20 |
|
|
|
| 2 |
A' |
643 |
583 |
17.46 |
|
|
|
| 3 |
A' |
434 |
394 |
20.77 |
|
|
|
| 4 |
A' |
193 |
175 |
7.35 |
|
|
|
| 5 |
A" |
758 |
687 |
708.21 |
|
|
|
| 6 |
A" |
548 |
496 |
1.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1780.1 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 1613.4 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/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
-0.313 |
-0.214 |
0.000 |
| F2 |
1.183 |
0.143 |
0.000 |
| F3 |
-0.313 |
0.119 |
1.590 |
| F4 |
-0.313 |
0.119 |
-1.590 |
Atom - Atom Distances (Å)
| |
S1 |
F2 |
F3 |
F4 |
| S1 | | 1.5378 | 1.6244 | 1.6244 |
F2 | 1.5378 | | 2.1832 | 2.1832 | F3 | 1.6244 | 2.1832 | | 3.1799 | F4 | 1.6244 | 2.1832 | 3.1799 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
S1 |
F3 |
87.279 |
|
F2 |
S1 |
F4 |
87.279 |
| F3 |
S1 |
F4 |
156.362 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.930 |
|
|
|
| 2 |
F |
-0.229 |
|
|
|
| 3 |
F |
-0.350 |
|
|
|
| 4 |
F |
-0.350 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.565 |
-0.550 |
0.000 |
0.788 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.337 |
-0.263 |
0.000 |
| y |
-0.263 |
-25.552 |
0.000 |
| z |
0.000 |
0.000 |
-32.756 |
|
| Traceless |
| | x | y | z |
| x |
2.817 |
-0.263 |
0.000 |
| y |
-0.263 |
3.994 |
0.000 |
| z |
0.000 |
0.000 |
-6.812 |
|
| Polar |
| 3z2-r2 | -13.623 |
| x2-y2 | -0.785 |
| xy | -0.263 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.762 |
0.066 |
0.000 |
| y |
0.066 |
2.254 |
0.000 |
| z |
0.000 |
0.000 |
3.944 |
<r2> (average value of r
2) Å
2
| <r2> |
80.052 |
| (<r2>)1/2 |
8.947 |
Jump to
S1C1
Energy calculated at HF/Def2TZVPP
| | hartrees |
| Energy at 0K | -695.892312 |
| Energy at 298.15K | |
| HF Energy | -695.892312 |
| Nuclear repulsion energy | 196.582713 |
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/Def2TZVPP
| 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 |
993 |
900 |
147.75 |
|
|
|
| 2 |
A1 |
622 |
563 |
3.12 |
|
|
|
| 3 |
A1 |
443 |
401 |
20.99 |
|
|
|
| 4 |
B1 |
155i |
141i |
4.69 |
|
|
|
| 5 |
B2 |
751 |
681 |
818.05 |
|
|
|
| 6 |
B2 |
566 |
513 |
1.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1609.4 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 1458.8 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 HF/Def2TZVPP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.000 |
0.397 |
| F2 |
0.000 |
0.000 |
-1.144 |
| F3 |
0.000 |
1.634 |
0.219 |
| F4 |
0.000 |
-1.634 |
0.219 |
Atom - Atom Distances (Å)
| |
S1 |
F2 |
F3 |
F4 |
| S1 | | 1.5403 | 1.6441 | 1.6441 |
F2 | 1.5403 | | 2.1283 | 2.1283 | F3 | 1.6441 | 2.1283 | | 3.2690 | F4 | 1.6441 | 2.1283 | 3.2690 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
S1 |
F3 |
83.814 |
|
F2 |
S1 |
F4 |
83.814 |
| F3 |
S1 |
F4 |
167.628 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.951 |
|
|
|
| 2 |
F |
-0.221 |
|
|
|
| 3 |
F |
-0.365 |
|
|
|
| 4 |
F |
-0.365 |
|
|
|
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 |
0.659 |
0.659 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.075 |
0.000 |
0.000 |
| y |
0.000 |
-33.542 |
0.000 |
| z |
0.000 |
0.000 |
-26.419 |
|
| Traceless |
| | x | y | z |
| x |
4.905 |
0.000 |
0.000 |
| y |
0.000 |
-7.795 |
0.000 |
| z |
0.000 |
0.000 |
2.890 |
|
| Polar |
| 3z2-r2 | 5.780 |
| x2-y2 | 8.467 |
| 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 |
2.299 |
0.000 |
0.000 |
| y |
0.000 |
3.959 |
0.000 |
| z |
0.000 |
0.000 |
2.739 |
<r2> (average value of r
2) Å
2
| <r2> |
80.654 |
| (<r2>)1/2 |
8.981 |