Jump to
S1C2
Energy calculated at B97D3/6-31+G**
| | hartrees |
| Energy at 0K | -697.509220 |
| Energy at 298.15K | -697.510117 |
| HF Energy | -697.509220 |
| Nuclear repulsion energy | 184.027807 |
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 B97D3/6-31+G**
| 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' |
767 |
754 |
103.88 |
|
|
|
| 2 |
A' |
523 |
514 |
10.03 |
|
|
|
| 3 |
A' |
298 |
293 |
11.86 |
|
|
|
| 4 |
A' |
123 |
121 |
10.48 |
|
|
|
| 5 |
A" |
654 |
643 |
458.48 |
|
|
|
| 6 |
A" |
397 |
391 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1381.2 cm
-1
Scaled (by 0.9828) Zero Point Vibrational Energy (zpe) 1357.4 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 B97D3/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
-0.338 |
-0.141 |
0.000 |
| F2 |
1.276 |
0.089 |
0.000 |
| F3 |
-0.338 |
0.081 |
1.712 |
| F4 |
-0.338 |
0.081 |
-1.712 |
Atom - Atom Distances (Å)
| |
S1 |
F2 |
F3 |
F4 |
| S1 | | 1.6297 | 1.7260 | 1.7260 |
F2 | 1.6297 | | 2.3521 | 2.3521 | F3 | 1.7260 | 2.3521 | | 3.4232 | F4 | 1.7260 | 2.3521 | 3.4232 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
S1 |
F3 |
88.764 |
|
F2 |
S1 |
F4 |
88.764 |
| F3 |
S1 |
F4 |
157.522 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.022 |
|
|
|
| 2 |
F |
-0.280 |
|
|
|
| 3 |
F |
-0.371 |
|
|
|
| 4 |
F |
-0.371 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.773 |
-0.533 |
0.000 |
0.939 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.885 |
0.030 |
0.000 |
| y |
0.030 |
-26.074 |
0.000 |
| z |
0.000 |
0.000 |
-33.542 |
|
| Traceless |
| | x | y | z |
| x |
2.924 |
0.030 |
0.000 |
| y |
0.030 |
4.139 |
0.000 |
| z |
0.000 |
0.000 |
-7.063 |
|
| Polar |
| 3z2-r2 | -14.126 |
| x2-y2 | -0.810 |
| xy | 0.030 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.578 |
0.075 |
0.000 |
| y |
0.075 |
2.663 |
0.000 |
| z |
0.000 |
0.000 |
6.027 |
<r2> (average value of r
2) Å
2
| <r2> |
89.772 |
| (<r2>)1/2 |
9.475 |
Jump to
S1C1
Energy calculated at B97D3/6-31+G**
| | hartrees |
| Energy at 0K | -697.508964 |
| Energy at 298.15K | |
| HF Energy | -697.508964 |
| Nuclear repulsion energy | 183.975650 |
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 B97D3/6-31+G**
| 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 |
765 |
752 |
103.73 |
|
|
|
| 2 |
A1 |
516 |
507 |
5.34 |
|
|
|
| 3 |
A1 |
298 |
292 |
11.64 |
|
|
|
| 4 |
B1 |
91i |
90i |
11.06 |
|
|
|
| 5 |
B2 |
665 |
653 |
478.09 |
|
|
|
| 6 |
B2 |
404 |
397 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1278.1 cm
-1
Scaled (by 0.9828) Zero Point Vibrational Energy (zpe) 1256.1 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 B97D3/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.000 |
0.360 |
| F2 |
0.000 |
0.000 |
-1.271 |
| F3 |
0.000 |
1.726 |
0.316 |
| F4 |
0.000 |
-1.726 |
0.316 |
Atom - Atom Distances (Å)
| |
S1 |
F2 |
F3 |
F4 |
| S1 | | 1.6306 | 1.7266 | 1.7266 |
F2 | 1.6306 | | 2.3447 | 2.3447 | F3 | 1.7266 | 2.3447 | | 3.4522 | F4 | 1.7266 | 2.3447 | 3.4522 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
S1 |
F3 |
87.692 |
|
F2 |
S1 |
F4 |
87.692 |
| F3 |
S1 |
F4 |
175.384 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.054 |
|
|
|
| 2 |
F |
-0.275 |
|
|
|
| 3 |
F |
-0.389 |
|
|
|
| 4 |
F |
-0.389 |
|
|
|
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 |
0.848 |
0.848 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.948 |
0.000 |
0.000 |
| y |
0.000 |
-33.914 |
0.000 |
| z |
0.000 |
0.000 |
-26.837 |
|
| Traceless |
| | x | y | z |
| x |
4.427 |
0.000 |
0.000 |
| y |
0.000 |
-7.521 |
0.000 |
| z |
0.000 |
0.000 |
3.094 |
|
| Polar |
| 3z2-r2 | 6.189 |
| x2-y2 | 7.965 |
| 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 |
2.631 |
0.000 |
0.000 |
| y |
0.000 |
6.143 |
0.000 |
| z |
0.000 |
0.000 |
3.592 |
<r2> (average value of r
2) Å
2
| <r2> |
90.083 |
| (<r2>)1/2 |
9.491 |