Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-31G(2df,p)
| hartrees |
Energy at 0K | -759.153741 |
Energy at 298.15K | |
HF Energy | -758.823331 |
Nuclear repulsion energy | 182.042105 |
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 B2PLYP=FULL/6-31G(2df,p)
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' |
555 |
555 |
0.00 |
|
|
|
2 |
A2" |
425 |
425 |
18.10 |
|
|
|
3 |
E' |
60i |
60i |
0.32 |
|
|
|
3 |
E' |
60i |
60i |
0.32 |
|
|
|
4 |
E' |
595 |
595 |
196.27 |
|
|
|
4 |
E' |
595 |
595 |
196.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1025.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1025.4 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 B2PLYP=FULL/6-31G(2df,p)
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.000 |
F2 |
0.000 |
1.742 |
0.000 |
F3 |
1.509 |
-0.871 |
0.000 |
F4 |
-1.509 |
-0.871 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7421 | 1.7421 | 1.7421 |
F2 | 1.7421 | | 3.0174 | 3.0174 | F3 | 1.7421 | 3.0174 | | 3.0174 | F4 | 1.7421 | 3.0174 | 3.0174 | |
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
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-31G(2df,p)
| hartrees |
Energy at 0K | -759.180517 |
Energy at 298.15K | -759.181862 |
HF Energy | -758.872632 |
Nuclear repulsion energy | 194.709735 |
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 B2PLYP=FULL/6-31G(2df,p)
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 |
752 |
752 |
40.43 |
|
|
|
2 |
A1 |
539 |
539 |
2.37 |
|
|
|
3 |
A1 |
319 |
319 |
10.83 |
|
|
|
4 |
B1 |
326 |
326 |
13.65 |
|
|
|
5 |
B2 |
735 |
735 |
388.89 |
|
|
|
6 |
B2 |
423 |
423 |
0.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1546.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1546.2 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 B2PLYP=FULL/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.365 |
F2 |
0.000 |
0.000 |
-1.252 |
F3 |
0.000 |
1.707 |
0.281 |
F4 |
0.000 |
-1.707 |
0.281 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.6176 | 1.7092 | 1.7092 |
F2 | 1.6176 | | 2.2944 | 2.2944 | F3 | 1.7092 | 2.2944 | | 3.4142 | F4 | 1.7092 | 2.2944 | 3.4142 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.165 |
|
F2 |
Cl1 |
F4 |
87.165 |
F3 |
Cl1 |
F4 |
174.329 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability