Jump to
S1C2
S1C3
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -99.207968 |
| Energy at 298.15K | -99.207236 |
| HF Energy | -99.207968 |
| Nuclear repulsion energy | 27.813532 |
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/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.075 |
| C2 |
0.000 |
0.000 |
-0.142 |
| N3 |
0.000 |
0.000 |
1.011 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9336 | 3.0860 |
C2 | 1.9336 | | 1.1524 | N3 | 3.0860 | 1.1524 | |
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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.599 |
|
|
|
| 2 |
C |
-0.091 |
|
|
|
| 3 |
N |
-0.508 |
|
|
|
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 |
-9.109 |
9.109 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.136 |
0.000 |
0.000 |
| y |
0.000 |
-14.136 |
0.000 |
| z |
0.000 |
0.000 |
1.207 |
|
| Traceless |
| | x | y | z |
| x |
-7.672 |
0.000 |
0.000 |
| y |
0.000 |
-7.672 |
0.000 |
| z |
0.000 |
0.000 |
15.343 |
|
| Polar |
| 3z2-r2 | 30.686 |
| 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 |
1.703 |
0.000 |
0.000 |
| y |
0.000 |
1.703 |
0.000 |
| z |
0.000 |
0.000 |
3.652 |
<r2> (average value of r
2) Å
2
| <r2> |
25.827 |
| (<r2>)1/2 |
5.082 |
Jump to
S1C1
S1C3
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -99.224462 |
| Energy at 298.15K | -99.223763 |
| HF Energy | -99.224462 |
| Nuclear repulsion energy | 28.624840 |
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/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
-0.010 |
1.862 |
0.000 |
| C2 |
0.005 |
-1.059 |
0.000 |
| N3 |
0.000 |
0.110 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9207 | 1.7523 |
C2 | 2.9207 | | 1.1684 | N3 | 1.7523 | 1.1684 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
0.051 |
|
Li1 |
N3 |
C2 |
179.915 |
| C2 |
Li1 |
N3 |
0.034 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.606 |
|
|
|
| 2 |
C |
0.156 |
|
|
|
| 3 |
N |
-0.762 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.047 |
8.316 |
0.000 |
8.316 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.981 |
-0.069 |
0.000 |
| y |
-0.069 |
-2.577 |
0.000 |
| z |
0.000 |
0.000 |
-13.982 |
|
| Traceless |
| | x | y | z |
| x |
-5.702 |
-0.069 |
0.000 |
| y |
-0.069 |
11.404 |
0.000 |
| z |
0.000 |
0.000 |
-5.702 |
|
| Polar |
| 3z2-r2 | -11.405 |
| x2-y2 | -11.404 |
| xy | -0.069 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.635 |
-0.011 |
0.000 |
| y |
-0.011 |
3.858 |
0.000 |
| z |
0.000 |
0.000 |
1.635 |
<r2> (average value of r
2) Å
2
| <r2> |
23.569 |
| (<r2>)1/2 |
4.855 |
Jump to
S1C1
S1C2
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -99.224462 |
| Energy at 298.15K | -99.223595 |
| HF Energy | -99.224462 |
| Nuclear repulsion energy | 28.628656 |
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/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.862 |
| C2 |
0.000 |
0.000 |
-1.059 |
| N3 |
0.000 |
0.000 |
0.110 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9202 | 1.7519 |
C2 | 2.9202 | | 1.1683 | N3 | 1.7519 | 1.1683 | |
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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.606 |
|
|
|
| 2 |
C |
0.156 |
|
|
|
| 3 |
N |
-0.762 |
|
|
|
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 |
8.314 |
8.314 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.981 |
0.000 |
0.000 |
| y |
0.000 |
-13.981 |
0.000 |
| z |
0.000 |
0.000 |
-2.582 |
|
| Traceless |
| | x | y | z |
| x |
-5.700 |
0.000 |
0.000 |
| y |
0.000 |
-5.700 |
0.000 |
| z |
0.000 |
0.000 |
11.399 |
|
| Polar |
| 3z2-r2 | 22.798 |
| 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 |
1.635 |
0.000 |
0.000 |
| y |
0.000 |
1.635 |
0.000 |
| z |
0.000 |
0.000 |
3.857 |
<r2> (average value of r
2) Å
2
| <r2> |
23.564 |
| (<r2>)1/2 |
4.854 |