Jump to
S1C2
Energy calculated at B97D3/6-311G**
| | hartrees |
| Energy at 0K | -697.592642 |
| Energy at 298.15K | -697.593508 |
| HF Energy | -697.592642 |
| Nuclear repulsion energy | 184.008069 |
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 B97D3/6-311G**
| 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' |
741 |
730 |
91.23 |
|
|
|
| 2 |
A' |
510 |
503 |
8.08 |
|
|
|
| 3 |
A' |
300 |
296 |
12.27 |
|
|
|
| 4 |
A' |
115 |
113 |
10.48 |
|
|
|
| 5 |
A" |
639 |
630 |
353.15 |
|
|
|
| 6 |
A" |
396 |
391 |
0.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1350.6 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 1331.2 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 B97D3/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
-0.338 |
-0.137 |
0.000 |
| F2 |
1.276 |
0.073 |
0.000 |
| F3 |
-0.338 |
0.085 |
1.712 |
| F4 |
-0.338 |
0.085 |
-1.712 |
Atom - Atom Distances (Å)
| |
S1 |
F2 |
F3 |
F4 |
| S1 | | 1.6279 | 1.7269 | 1.7269 |
F2 | 1.6279 | | 2.3533 | 2.3533 | F3 | 1.7269 | 2.3533 | | 3.4249 | F4 | 1.7269 | 2.3533 | 3.4249 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
S1 |
F3 |
88.953 |
|
F2 |
S1 |
F4 |
88.953 |
| F3 |
S1 |
F4 |
157.359 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.949 |
|
|
|
| 2 |
F |
-0.261 |
|
|
|
| 3 |
F |
-0.344 |
|
|
|
| 4 |
F |
-0.344 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.841 |
-0.511 |
0.000 |
0.984 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.636 |
0.033 |
0.000 |
| y |
0.033 |
-25.573 |
0.000 |
| z |
0.000 |
0.000 |
-33.065 |
|
| Traceless |
| | x | y | z |
| x |
2.683 |
0.033 |
0.000 |
| y |
0.033 |
4.278 |
0.000 |
| z |
0.000 |
0.000 |
-6.961 |
|
| Polar |
| 3z2-r2 | -13.921 |
| x2-y2 | -1.063 |
| xy | 0.033 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.864 |
0.069 |
0.000 |
| y |
0.069 |
1.839 |
0.000 |
| z |
0.000 |
0.000 |
5.061 |
<r2> (average value of r
2) Å
2
| <r2> |
89.561 |
| (<r2>)1/2 |
9.464 |
Jump to
S1C1
Energy calculated at B97D3/6-311G**
| | hartrees |
| Energy at 0K | -697.592425 |
| Energy at 298.15K | |
| HF Energy | -697.592425 |
| Nuclear repulsion energy | 183.888894 |
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 B97D3/6-311G**
| 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 |
738 |
728 |
90.90 |
|
|
|
| 2 |
A1 |
504 |
497 |
3.90 |
|
|
|
| 3 |
A1 |
300 |
295 |
11.85 |
|
|
|
| 4 |
B1 |
83i |
81i |
9.81 |
|
|
|
| 5 |
B2 |
649 |
640 |
366.13 |
|
|
|
| 6 |
B2 |
403 |
397 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1255.6 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 1237.7 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 B97D3/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.000 |
0.358 |
| F2 |
0.000 |
0.000 |
-1.271 |
| F3 |
0.000 |
1.728 |
0.318 |
| F4 |
0.000 |
-1.728 |
0.318 |
Atom - Atom Distances (Å)
| |
S1 |
F2 |
F3 |
F4 |
| S1 | | 1.6289 | 1.7283 | 1.7283 |
F2 | 1.6289 | | 2.3471 | 2.3471 | F3 | 1.7283 | 2.3471 | | 3.4556 | F4 | 1.7283 | 2.3471 | 3.4556 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
S1 |
F3 |
87.821 |
|
F2 |
S1 |
F4 |
87.821 |
| F3 |
S1 |
F4 |
175.642 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.954 |
|
|
|
| 2 |
F |
-0.258 |
|
|
|
| 3 |
F |
-0.348 |
|
|
|
| 4 |
F |
-0.348 |
|
|
|
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 |
0.903 |
0.903 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.456 |
0.000 |
0.000 |
| y |
0.000 |
-33.372 |
0.000 |
| z |
0.000 |
0.000 |
-26.587 |
|
| Traceless |
| | x | y | z |
| x |
4.524 |
0.000 |
0.000 |
| y |
0.000 |
-7.350 |
0.000 |
| z |
0.000 |
0.000 |
2.826 |
|
| Polar |
| 3z2-r2 | 5.652 |
| x2-y2 | 7.916 |
| 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 |
1.823 |
0.000 |
0.000 |
| y |
0.000 |
5.171 |
0.000 |
| z |
0.000 |
0.000 |
2.874 |
<r2> (average value of r
2) Å
2
| <r2> |
89.924 |
| (<r2>)1/2 |
9.483 |