Jump to
S2C1
Energy calculated at LSDA/3-21G
| hartrees |
Energy at 0K | -235.269869 |
Energy at 298.15K | -235.269595 |
HF Energy | -235.269869 |
Nuclear repulsion energy | 62.725089 |
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/3-21G
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.623 |
F2 |
0.000 |
1.058 |
-0.208 |
F3 |
0.000 |
-1.058 |
-0.208 |
Atom - Atom Distances (Å)
|
C1 |
F2 |
F3 |
C1 | | 1.3455 | 1.3455 |
F2 | 1.3455 | | 2.1169 | F3 | 1.3455 | 2.1169 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
C1 |
F3 |
103.757 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.398 |
|
|
|
2 |
F |
-0.199 |
|
|
|
3 |
F |
-0.199 |
|
|
|
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 |
-0.786 |
0.786 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-13.789 |
0.000 |
0.000 |
y |
0.000 |
-15.721 |
0.000 |
z |
0.000 |
0.000 |
-16.779 |
|
Traceless |
| x | y | z |
x |
2.461 |
0.000 |
0.000 |
y |
0.000 |
-0.437 |
0.000 |
z |
0.000 |
0.000 |
-2.024 |
|
Polar |
3z2-r2 | -4.048 |
x2-y2 | 1.932 |
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 |
1.163 |
0.000 |
0.000 |
y |
0.000 |
2.031 |
0.000 |
z |
0.000 |
0.000 |
1.212 |
<r2> (average value of r
2) Å
2
<r2> |
32.908 |
(<r2>)1/2 |
5.737 |
Jump to
S1C1
Energy calculated at LSDA/3-21G
| hartrees |
Energy at 0K | -235.186136 |
Energy at 298.15K | -235.185797 |
Nuclear repulsion energy | 60.748450 |
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/3-21G
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.493 |
F2 |
0.000 |
1.173 |
-0.164 |
F3 |
0.000 |
-1.173 |
-0.164 |
Atom - Atom Distances (Å)
|
C1 |
F2 |
F3 |
C1 | | 1.3452 | 1.3452 |
F2 | 1.3452 | | 2.3469 | F3 | 1.3452 | 2.3469 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
C1 |
F3 |
121.461 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.376 |
|
|
|
2 |
F |
-0.188 |
|
|
|
3 |
F |
-0.188 |
|
|
|
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 |
-0.003 |
0.003 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.804 |
0.000 |
0.000 |
y |
0.000 |
-15.767 |
0.000 |
z |
0.000 |
0.000 |
-14.588 |
|
Traceless |
| x | y | z |
x |
0.374 |
0.000 |
0.000 |
y |
0.000 |
-1.071 |
0.000 |
z |
0.000 |
0.000 |
0.697 |
|
Polar |
3z2-r2 | 1.395 |
x2-y2 | 0.963 |
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 |
0.710 |
0.000 |
0.000 |
y |
0.000 |
1.964 |
0.000 |
z |
0.000 |
0.000 |
1.147 |
<r2> (average value of r
2) Å
2
<r2> |
36.135 |
(<r2>)1/2 |
6.011 |