Jump to
S1C2
Energy calculated at PBE1PBE/cc-pCVTZ
| hartrees |
Energy at 0K | -759.184849 |
Energy at 298.15K | |
HF Energy | -759.184849 |
Nuclear repulsion energy | 184.823590 |
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 PBE1PBE/cc-pCVTZ
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' |
589 |
589 |
0.00 |
|
|
|
2 |
A2" |
452 |
452 |
26.06 |
|
|
|
3 |
E' |
602 |
602 |
307.94 |
|
|
|
3 |
E' |
602 |
602 |
307.93 |
|
|
|
4 |
E' |
141i |
141i |
2.76 |
|
|
|
4 |
E' |
141i |
141i |
2.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 981.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 981.5 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 PBE1PBE/cc-pCVTZ
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.000 |
F2 |
0.000 |
1.716 |
0.000 |
F3 |
1.486 |
-0.858 |
0.000 |
F4 |
-1.486 |
-0.858 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7159 | 1.7159 | 1.7159 |
F2 | 1.7159 | | 2.9720 | 2.9720 | F3 | 1.7159 | 2.9720 | | 2.9720 | F4 | 1.7159 | 2.9720 | 2.9720 | |
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 PBE1PBE/cc-pCVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.793 |
|
|
|
2 |
F |
-0.264 |
|
|
|
3 |
F |
-0.264 |
|
|
|
4 |
F |
-0.264 |
|
|
|
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 |
-29.305 |
0.000 |
0.000 |
y |
0.000 |
-29.305 |
0.000 |
z |
0.000 |
0.000 |
-26.195 |
|
Traceless |
| x | y | z |
x |
-1.555 |
0.000 |
0.000 |
y |
0.000 |
-1.555 |
0.000 |
z |
0.000 |
0.000 |
3.109 |
|
Polar |
3z2-r2 | 6.218 |
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 |
4.751 |
0.000 |
0.000 |
y |
0.000 |
4.751 |
0.000 |
z |
0.000 |
0.000 |
1.753 |
<r2> (average value of r
2) Å
2
<r2> |
97.150 |
(<r2>)1/2 |
9.856 |
Jump to
S1C1
Energy calculated at PBE1PBE/cc-pCVTZ
| hartrees |
Energy at 0K | -759.222284 |
Energy at 298.15K | -759.223753 |
HF Energy | -759.222284 |
Nuclear repulsion energy | 196.986719 |
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 PBE1PBE/cc-pCVTZ
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 |
798 |
798 |
56.32 |
|
|
|
2 |
A1 |
563 |
563 |
4.14 |
|
|
|
3 |
A1 |
340 |
340 |
12.85 |
|
|
|
4 |
B1 |
347 |
347 |
16.37 |
|
|
|
5 |
B2 |
746 |
746 |
504.76 |
|
|
|
6 |
B2 |
447 |
447 |
0.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1620.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1620.2 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 PBE1PBE/cc-pCVTZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.356 |
F2 |
0.000 |
0.000 |
-1.240 |
F3 |
0.000 |
1.688 |
0.283 |
F4 |
0.000 |
-1.688 |
0.283 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.5958 | 1.6895 | 1.6895 |
F2 | 1.5958 | | 2.2734 | 2.2734 | F3 | 1.6895 | 2.2734 | | 3.3758 | F4 | 1.6895 | 2.2734 | 3.3758 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.529 |
|
F2 |
Cl1 |
F4 |
87.529 |
F3 |
Cl1 |
F4 |
175.059 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pCVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.729 |
|
|
|
2 |
F |
-0.124 |
|
|
|
3 |
F |
-0.302 |
|
|
|
4 |
F |
-0.302 |
|
|
|
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 |
0.612 |
0.612 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.939 |
0.000 |
0.000 |
y |
0.000 |
-32.139 |
0.000 |
z |
0.000 |
0.000 |
-25.183 |
|
Traceless |
| x | y | z |
x |
2.722 |
0.000 |
0.000 |
y |
0.000 |
-6.578 |
0.000 |
z |
0.000 |
0.000 |
3.856 |
|
Polar |
3z2-r2 | 7.713 |
x2-y2 | 6.200 |
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 |
1.800 |
0.000 |
0.000 |
y |
0.000 |
4.907 |
0.000 |
z |
0.000 |
0.000 |
2.877 |
<r2> (average value of r
2) Å
2
<r2> |
86.048 |
(<r2>)1/2 |
9.276 |