Jump to
S1C2
Energy calculated at M06-2X/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -759.458711 |
Energy at 298.15K | |
HF Energy | -759.458711 |
Nuclear repulsion energy | 185.817039 |
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 M06-2X/6-311+G(3df,2p)
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' |
611 |
611 |
0.01 |
27.76 |
0.11 |
0.19 |
2 |
A2" |
462 |
462 |
28.35 |
0.00 |
0.75 |
0.86 |
3 |
E' |
608 |
608 |
374.02 |
16.38 |
0.75 |
0.86 |
3 |
E' |
608 |
608 |
374.61 |
16.27 |
0.75 |
0.86 |
4 |
E' |
184i |
184i |
9.26 |
4.31 |
0.75 |
0.86 |
4 |
E' |
184i |
184i |
9.27 |
4.28 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 959.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 959.9 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 M06-2X/6-311+G(3df,2p)
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.000 |
F2 |
0.000 |
1.707 |
0.000 |
F3 |
1.478 |
-0.853 |
0.000 |
F4 |
-1.478 |
-0.853 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7067 | 1.7067 | 1.7067 |
F2 | 1.7067 | | 2.9561 | 2.9561 | F3 | 1.7067 | 2.9561 | | 2.9561 | F4 | 1.7067 | 2.9561 | 2.9561 | |
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 M06-2X/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.023 |
|
|
|
2 |
F |
-0.341 |
|
|
|
3 |
F |
-0.341 |
|
|
|
4 |
F |
-0.341 |
|
|
|
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 |
-30.076 |
0.000 |
0.000 |
y |
0.000 |
-30.076 |
0.000 |
z |
0.000 |
0.000 |
-26.629 |
|
Traceless |
| x | y | z |
x |
-1.724 |
0.000 |
0.000 |
y |
0.000 |
-1.724 |
0.000 |
z |
0.000 |
0.000 |
3.447 |
|
Polar |
3z2-r2 | 6.894 |
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 |
5.396 |
0.000 |
0.000 |
y |
0.000 |
5.395 |
0.000 |
z |
0.000 |
0.000 |
2.435 |
<r2> (average value of r
2) Å
2
<r2> |
96.714 |
(<r2>)1/2 |
9.834 |
Jump to
S1C1
Energy calculated at M06-2X/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -759.510799 |
Energy at 298.15K | |
HF Energy | -759.510799 |
Nuclear repulsion energy | 198.153721 |
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 M06-2X/6-311+G(3df,2p)
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 |
838 |
838 |
51.50 |
12.58 |
0.12 |
0.21 |
2 |
A1 |
578 |
578 |
2.96 |
24.54 |
0.36 |
0.53 |
3 |
A1 |
364 |
364 |
15.36 |
0.59 |
0.15 |
0.26 |
4 |
B1 |
352 |
352 |
17.88 |
0.04 |
0.75 |
0.86 |
5 |
B2 |
733 |
733 |
564.41 |
0.34 |
0.75 |
0.86 |
6 |
B2 |
467 |
467 |
0.86 |
1.43 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1665.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1665.3 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 M06-2X/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.366 |
F2 |
0.000 |
0.000 |
-1.220 |
F3 |
0.000 |
1.681 |
0.264 |
F4 |
0.000 |
-1.681 |
0.264 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.5859 | 1.6846 | 1.6846 |
F2 | 1.5859 | | 2.2422 | 2.2422 | F3 | 1.6846 | 2.2422 | | 3.3630 | F4 | 1.6846 | 2.2422 | 3.3630 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
86.510 |
|
F2 |
Cl1 |
F4 |
86.510 |
F3 |
Cl1 |
F4 |
173.020 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.945 |
|
|
|
2 |
F |
-0.140 |
|
|
|
3 |
F |
-0.403 |
|
|
|
4 |
F |
-0.403 |
|
|
|
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 |
0.661 |
0.661 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.312 |
0.000 |
0.000 |
y |
0.000 |
-32.988 |
0.000 |
z |
0.000 |
0.000 |
-25.589 |
|
Traceless |
| x | y | z |
x |
2.977 |
0.000 |
0.000 |
y |
0.000 |
-7.038 |
0.000 |
z |
0.000 |
0.000 |
4.060 |
|
Polar |
3z2-r2 | 8.121 |
x2-y2 | 6.676 |
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 |
2.424 |
0.000 |
0.000 |
y |
0.000 |
5.428 |
0.000 |
z |
0.000 |
0.000 |
3.379 |
<r2> (average value of r
2) Å
2
<r2> |
85.486 |
(<r2>)1/2 |
9.246 |