Jump to
S1C2
S1C3
Energy calculated at HF/6-311G**
| hartrees |
Energy at 0K | -99.799532 |
Energy at 298.15K | -99.798654 |
HF Energy | -99.799532 |
Nuclear repulsion energy | 28.020986 |
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 HF/6-311G**
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Li1 |
0.000 |
0.000 |
-2.067 |
C2 |
0.000 |
0.000 |
-0.138 |
N3 |
0.000 |
0.000 |
1.004 |
Atom - Atom Distances (Å)
|
Li1 |
C2 |
N3 |
Li1 | | 1.9289 | 3.0707 |
C2 | 1.9289 | | 1.1419 | N3 | 3.0707 | 1.1419 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li1 |
C2 |
N3 |
180.000 |
|
Li1 |
N3 |
C2 |
0.000 |
C2 |
Li1 |
N3 |
0.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Li |
0.660 |
|
|
|
2 |
C |
-0.290 |
|
|
|
3 |
N |
-0.370 |
|
|
|
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 |
-9.395 |
9.395 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.140 |
0.000 |
0.000 |
y |
0.000 |
-14.140 |
0.000 |
z |
0.000 |
0.000 |
1.516 |
|
Traceless |
| x | y | z |
x |
-7.828 |
0.000 |
0.000 |
y |
0.000 |
-7.828 |
0.000 |
z |
0.000 |
0.000 |
15.657 |
|
Polar |
3z2-r2 | 31.313 |
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 |
2.026 |
0.000 |
0.000 |
y |
0.000 |
2.026 |
0.000 |
z |
0.000 |
0.000 |
3.826 |
<r2> (average value of r
2) Å
2
<r2> |
25.557 |
(<r2>)1/2 |
5.055 |
Jump to
S1C1
S1C3
Energy calculated at HF/6-311G**
| hartrees |
Energy at 0K | -99.809644 |
Energy at 298.15K | -99.808843 |
HF Energy | -99.809644 |
Nuclear repulsion energy | 28.763727 |
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 HF/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Li1 |
0.001 |
1.868 |
0.000 |
C2 |
-0.001 |
-1.054 |
0.000 |
N3 |
0.000 |
0.103 |
0.000 |
Atom - Atom Distances (Å)
|
Li1 |
C2 |
N3 |
Li1 | | 2.9220 | 1.7649 |
C2 | 2.9220 | | 1.1571 | N3 | 1.7649 | 1.1571 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li1 |
C2 |
N3 |
0.006 |
|
Li1 |
N3 |
C2 |
179.990 |
C2 |
Li1 |
N3 |
0.004 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Li |
0.663 |
|
|
|
2 |
C |
-0.070 |
|
|
|
3 |
N |
-0.593 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.006 |
8.754 |
0.000 |
8.754 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.072 |
0.009 |
0.000 |
y |
0.009 |
-2.128 |
0.000 |
z |
0.000 |
0.000 |
-14.072 |
|
Traceless |
| x | y | z |
x |
-5.972 |
0.009 |
0.000 |
y |
0.009 |
11.944 |
0.000 |
z |
0.000 |
0.000 |
-5.972 |
|
Polar |
3z2-r2 | -11.944 |
x2-y2 | -11.944 |
xy | 0.009 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.059 |
0.001 |
0.000 |
y |
0.001 |
3.930 |
0.000 |
z |
0.000 |
0.000 |
2.059 |
<r2> (average value of r
2) Å
2
<r2> |
23.511 |
(<r2>)1/2 |
4.849 |
Jump to
S1C1
S1C2
Energy calculated at HF/6-311G**
| hartrees |
Energy at 0K | -99.809644 |
Energy at 298.15K | -99.808599 |
HF Energy | -99.809644 |
Nuclear repulsion energy | 28.763311 |
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 HF/6-311G**
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Li1 |
0.000 |
0.000 |
1.868 |
C2 |
0.000 |
0.000 |
-1.054 |
N3 |
0.000 |
0.000 |
0.103 |
Atom - Atom Distances (Å)
|
Li1 |
C2 |
N3 |
Li1 | | 2.9221 | 1.7650 |
C2 | 2.9221 | | 1.1571 | N3 | 1.7650 | 1.1571 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li1 |
C2 |
N3 |
0.000 |
|
Li1 |
N3 |
C2 |
180.000 |
C2 |
Li1 |
N3 |
0.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Li |
0.663 |
|
|
|
2 |
C |
-0.070 |
|
|
|
3 |
N |
-0.593 |
|
|
|
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 |
8.754 |
8.754 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.072 |
0.000 |
0.000 |
y |
0.000 |
-14.072 |
0.000 |
z |
0.000 |
0.000 |
-2.127 |
|
Traceless |
| x | y | z |
x |
-5.972 |
0.000 |
0.000 |
y |
0.000 |
-5.972 |
0.000 |
z |
0.000 |
0.000 |
11.945 |
|
Polar |
3z2-r2 | 23.890 |
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 |
2.059 |
0.000 |
0.000 |
y |
0.000 |
2.059 |
0.000 |
z |
0.000 |
0.000 |
3.930 |
<r2> (average value of r
2) Å
2
<r2> |
23.512 |
(<r2>)1/2 |
4.849 |