Jump to
S1C2
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -695.881160 |
| Energy at 298.15K | -695.882599 |
| HF Energy | -695.881160 |
| Nuclear repulsion energy | 195.590747 |
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/daug-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 |
A' |
975 |
882 |
131.81 |
|
|
|
| 2 |
A' |
641 |
580 |
17.50 |
|
|
|
| 3 |
A' |
425 |
385 |
20.26 |
|
|
|
| 4 |
A' |
198 |
180 |
7.56 |
|
|
|
| 5 |
A" |
742 |
671 |
689.38 |
|
|
|
| 6 |
A" |
538 |
487 |
1.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1759.5 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 1591.6 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/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
-0.311 |
-0.206 |
0.000 |
| F2 |
1.176 |
0.173 |
0.000 |
| F3 |
-0.311 |
0.096 |
1.603 |
| F4 |
-0.311 |
0.096 |
-1.603 |
Atom - Atom Distances (Å)
| |
S1 |
F2 |
F3 |
F4 |
| S1 | | 1.5347 | 1.6317 | 1.6317 |
F2 | 1.5347 | | 2.1885 | 2.1885 | F3 | 1.6317 | 2.1885 | | 3.2070 | F4 | 1.6317 | 2.1885 | 3.2070 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
S1 |
F3 |
87.386 |
|
F2 |
S1 |
F4 |
87.386 |
| F3 |
S1 |
F4 |
158.666 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
2.123 |
|
|
|
| 2 |
F |
-0.821 |
|
|
|
| 3 |
F |
-0.651 |
|
|
|
| 4 |
F |
-0.651 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.554 |
-0.586 |
0.000 |
0.806 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.494 |
-0.236 |
0.000 |
| y |
-0.236 |
-25.764 |
0.000 |
| z |
0.000 |
0.000 |
-32.959 |
|
| Traceless |
| | x | y | z |
| x |
2.868 |
-0.236 |
0.000 |
| y |
-0.236 |
3.962 |
0.000 |
| z |
0.000 |
0.000 |
-6.830 |
|
| Polar |
| 3z2-r2 | -13.660 |
| x2-y2 | -0.730 |
| xy | -0.236 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.301 |
0.042 |
0.000 |
| y |
0.042 |
2.898 |
0.000 |
| z |
0.000 |
0.000 |
4.436 |
<r2> (average value of r
2) Å
2
| <r2> |
80.879 |
| (<r2>)1/2 |
8.993 |
Jump to
S1C1
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -695.879815 |
| Energy at 298.15K | |
| HF Energy | -695.879815 |
| Nuclear repulsion energy | 195.420616 |
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/daug-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 |
985 |
891 |
134.92 |
|
|
|
| 2 |
A1 |
618 |
559 |
2.31 |
|
|
|
| 3 |
A1 |
434 |
392 |
20.73 |
|
|
|
| 4 |
B1 |
162i |
147i |
5.13 |
|
|
|
| 5 |
B2 |
734 |
664 |
812.53 |
|
|
|
| 6 |
B2 |
558 |
505 |
1.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1582.9 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 1431.9 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/daug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.000 |
0.361 |
| F2 |
0.000 |
0.000 |
-1.170 |
| F3 |
0.000 |
1.634 |
0.264 |
| F4 |
0.000 |
-1.634 |
0.264 |
Atom - Atom Distances (Å)
| |
S1 |
F2 |
F3 |
F4 |
| S1 | | 1.5308 | 1.6372 | 1.6372 |
F2 | 1.5308 | | 2.1738 | 2.1738 | F3 | 1.6372 | 2.1738 | | 3.2685 | F4 | 1.6372 | 2.1738 | 3.2685 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
S1 |
F3 |
86.587 |
|
F2 |
S1 |
F4 |
86.587 |
| F3 |
S1 |
F4 |
173.175 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
2.182 |
|
|
|
| 2 |
F |
-0.840 |
|
|
|
| 3 |
F |
-0.671 |
|
|
|
| 4 |
F |
-0.671 |
|
|
|
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 |
0.657 |
0.657 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.275 |
0.000 |
0.000 |
| y |
0.000 |
-33.853 |
0.000 |
| z |
0.000 |
0.000 |
-26.557 |
|
| Traceless |
| | x | y | z |
| x |
4.930 |
0.000 |
0.000 |
| y |
0.000 |
-7.937 |
0.000 |
| z |
0.000 |
0.000 |
3.007 |
|
| Polar |
| 3z2-r2 | 6.014 |
| x2-y2 | 8.578 |
| 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 |
2.928 |
0.000 |
0.000 |
| y |
0.000 |
4.456 |
0.000 |
| z |
0.000 |
0.000 |
3.273 |
<r2> (average value of r
2) Å
2
| <r2> |
81.564 |
| (<r2>)1/2 |
9.031 |