Jump to
S2C1
Energy calculated at LSDA/6-311G*
| hartrees |
Energy at 0K | -236.634118 |
Energy at 298.15K | -236.633889 |
Nuclear repulsion energy | 64.857614 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at LSDA/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.598 |
F2 |
0.000 |
1.026 |
-0.199 |
F3 |
0.000 |
-1.026 |
-0.199 |
Atom - Atom Distances (Å)
|
C1 |
F2 |
F3 |
C1 | | 1.2995 | 1.2995 |
F2 | 1.2995 | | 2.0528 | F3 | 1.2995 | 2.0528 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
C1 |
F3 |
104.339 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.117 |
|
|
|
2 |
F |
-0.058 |
|
|
|
3 |
F |
-0.058 |
|
|
|
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 |
-0.816 |
0.816 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.320 |
0.000 |
0.000 |
y |
0.000 |
-15.683 |
0.000 |
z |
0.000 |
0.000 |
-17.110 |
|
Traceless |
| x | y | z |
x |
2.076 |
0.000 |
0.000 |
y |
0.000 |
0.032 |
0.000 |
z |
0.000 |
0.000 |
-2.109 |
|
Polar |
3z2-r2 | -4.217 |
x2-y2 | 1.363 |
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 |
1.580 |
0.000 |
0.000 |
y |
0.000 |
2.303 |
0.000 |
z |
0.000 |
0.000 |
1.590 |
<r2> (average value of r
2) Å
2
<r2> |
0.000 |
(<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at LSDA/6-311G*
| hartrees |
Energy at 0K | -236.544010 |
Energy at 298.15K | -236.543697 |
Nuclear repulsion energy | 62.622369 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at LSDA/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.494 |
F2 |
0.000 |
1.131 |
-0.165 |
F3 |
0.000 |
-1.131 |
-0.165 |
Atom - Atom Distances (Å)
|
C1 |
F2 |
F3 |
C1 | | 1.3086 | 1.3086 |
F2 | 1.3086 | | 2.2619 | F3 | 1.3086 | 2.2619 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
C1 |
F3 |
119.583 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.200 |
|
|
|
2 |
F |
-0.100 |
|
|
|
3 |
F |
-0.100 |
|
|
|
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 |
0.146 |
0.146 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-15.291 |
0.000 |
0.000 |
y |
0.000 |
-15.912 |
0.000 |
z |
0.000 |
0.000 |
-14.838 |
|
Traceless |
| x | y | z |
x |
0.084 |
0.000 |
0.000 |
y |
0.000 |
-0.848 |
0.000 |
z |
0.000 |
0.000 |
0.764 |
|
Polar |
3z2-r2 | 1.527 |
x2-y2 | 0.621 |
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 |
1.164 |
0.000 |
0.000 |
y |
0.000 |
2.152 |
0.000 |
z |
0.000 |
0.000 |
1.477 |
<r2> (average value of r
2) Å
2
<r2> |
34.558 |
(<r2>)1/2 |
5.879 |