Jump to
S1C2
Energy calculated at SVWN/6-31G(2df,p)
| hartrees |
Energy at 0K | -757.012665 |
Energy at 298.15K | |
HF Energy | -757.012665 |
Nuclear repulsion energy | 184.090276 |
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 SVWN/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' |
584 |
575 |
0.00 |
|
|
|
2 |
A2" |
433 |
426 |
14.92 |
|
|
|
3 |
E' |
79i |
78i |
0.29 |
|
|
|
3 |
E' |
79i |
78i |
0.29 |
|
|
|
4 |
E' |
638 |
629 |
198.90 |
|
|
|
4 |
E' |
638 |
629 |
198.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1067.2 cm
-1
Scaled (by 0.9852) Zero Point Vibrational Energy (zpe) 1051.4 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 SVWN/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 |
1.723 |
0.000 |
F3 |
1.492 |
-0.861 |
0.000 |
F4 |
-1.492 |
-0.861 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7227 | 1.7227 | 1.7227 |
F2 | 1.7227 | | 2.9838 | 2.9838 | F3 | 1.7227 | 2.9838 | | 2.9838 | F4 | 1.7227 | 2.9838 | 2.9838 | |
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
Charges from optimized geometry at SVWN/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.600 |
|
|
|
2 |
F |
-0.200 |
|
|
|
3 |
F |
-0.200 |
|
|
|
4 |
F |
-0.200 |
|
|
|
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 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-27.809 |
0.000 |
0.000 |
y |
0.000 |
-27.809 |
0.000 |
z |
0.000 |
0.000 |
-25.812 |
|
Traceless |
| x | y | z |
x |
-0.999 |
0.000 |
0.000 |
y |
0.000 |
-0.999 |
0.000 |
z |
0.000 |
0.000 |
1.997 |
|
Polar |
3z2-r2 | 3.994 |
x2-y2 | 0.000 |
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 |
4.722 |
0.000 |
0.000 |
y |
0.000 |
4.722 |
0.000 |
z |
0.000 |
0.000 |
2.104 |
<r2> (average value of r
2) Å
2
<r2> |
97.082 |
(<r2>)1/2 |
9.853 |
Jump to
S1C1
Energy calculated at SVWN/6-31G(2df,p)
| hartrees |
Energy at 0K | -757.035696 |
Energy at 298.15K | -757.037034 |
HF Energy | -757.035696 |
Nuclear repulsion energy | 195.966930 |
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 SVWN/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 |
753 |
741 |
46.39 |
|
|
|
2 |
A1 |
557 |
549 |
3.89 |
|
|
|
3 |
A1 |
303 |
298 |
7.86 |
|
|
|
4 |
B1 |
326 |
321 |
10.67 |
|
|
|
5 |
B2 |
768 |
757 |
352.55 |
|
|
|
6 |
B2 |
408 |
402 |
0.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1557.5 cm
-1
Scaled (by 0.9852) Zero Point Vibrational Energy (zpe) 1534.4 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 SVWN/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.360 |
F2 |
0.000 |
0.000 |
-1.256 |
F3 |
0.000 |
1.690 |
0.288 |
F4 |
0.000 |
-1.690 |
0.288 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.6155 | 1.6917 | 1.6917 |
F2 | 1.6155 | | 2.2892 | 2.2892 | F3 | 1.6917 | 2.2892 | | 3.3803 | F4 | 1.6917 | 2.2892 | 3.3803 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.576 |
|
F2 |
Cl1 |
F4 |
87.576 |
F3 |
Cl1 |
F4 |
175.152 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at SVWN/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.546 |
|
|
|
2 |
F |
-0.088 |
|
|
|
3 |
F |
-0.229 |
|
|
|
4 |
F |
-0.229 |
|
|
|
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 |
0.558 |
0.558 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.576 |
0.000 |
0.000 |
y |
0.000 |
-30.186 |
0.000 |
z |
0.000 |
0.000 |
-24.805 |
|
Traceless |
| x | y | z |
x |
1.920 |
0.000 |
0.000 |
y |
0.000 |
-4.996 |
0.000 |
z |
0.000 |
0.000 |
3.076 |
|
Polar |
3z2-r2 | 6.153 |
x2-y2 | 4.611 |
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 |
2.107 |
0.000 |
0.000 |
y |
0.000 |
4.933 |
0.000 |
z |
0.000 |
0.000 |
3.093 |
<r2> (average value of r
2) Å
2
<r2> |
86.080 |
(<r2>)1/2 |
9.278 |