Jump to
S1C2
S1C3
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -99.764263 |
| Energy at 298.15K | -99.763474 |
| HF Energy | -99.764263 |
| Nuclear repulsion energy | 27.543602 |
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 B1B95/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.068 |
| C2 |
0.000 |
0.000 |
-0.154 |
| N3 |
0.000 |
0.000 |
1.018 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9142 | 3.0860 |
C2 | 1.9142 | | 1.1718 | N3 | 3.0860 | 1.1718 | |
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 B1B95/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.531 |
|
|
|
| 2 |
C |
-0.073 |
|
|
|
| 3 |
N |
-0.458 |
|
|
|
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 |
-8.600 |
8.600 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.257 |
0.000 |
0.000 |
| y |
0.000 |
-14.257 |
0.000 |
| z |
0.000 |
0.000 |
1.056 |
|
| Traceless |
| | x | y | z |
| x |
-7.656 |
0.000 |
0.000 |
| y |
0.000 |
-7.656 |
0.000 |
| z |
0.000 |
0.000 |
15.312 |
|
| Polar |
| 3z2-r2 | 30.624 |
| 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 |
2.087 |
0.000 |
0.000 |
| y |
0.000 |
2.087 |
0.000 |
| z |
0.000 |
0.000 |
3.993 |
<r2> (average value of r
2) Å
2
| <r2> |
25.943 |
| (<r2>)1/2 |
5.093 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -99.748045 |
| Energy at 298.15K | |
| HF Energy | -99.748045 |
| Nuclear repulsion energy | 25.987192 |
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 B1B95/3-21G*
Geometric Data calculated at B1B95/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.472 |
-0.539 |
0.000 |
| C2 |
-0.736 |
-0.377 |
0.000 |
| N3 |
0.000 |
0.555 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.2137 | 1.8336 |
C2 | 2.2137 | | 1.1875 | N3 | 1.8336 | 1.1875 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
55.886 |
|
Li1 |
N3 |
C2 |
91.689 |
| C2 |
Li1 |
N3 |
32.425 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.518 |
|
|
|
| 2 |
C |
0.061 |
|
|
|
| 3 |
N |
-0.579 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
8.385 |
-1.722 |
0.000 |
8.561 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-0.572 |
-1.821 |
0.000 |
| y |
-1.821 |
-15.505 |
0.000 |
| z |
0.000 |
0.000 |
-14.657 |
|
| Traceless |
| | x | y | z |
| x |
14.509 |
-1.821 |
0.000 |
| y |
-1.821 |
-7.890 |
0.000 |
| z |
0.000 |
0.000 |
-6.619 |
|
| Polar |
| 3z2-r2 | -13.238 |
| x2-y2 | 14.933 |
| xy | -1.821 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.087 |
0.000 |
0.000 |
| y |
0.000 |
2.087 |
0.000 |
| z |
0.000 |
0.000 |
3.993 |
<r2> (average value of r
2) Å
2
| <r2> |
26.307 |
| (<r2>)1/2 |
5.129 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -99.773598 |
| Energy at 298.15K | -99.772595 |
| HF Energy | -99.773598 |
| Nuclear repulsion energy | 28.324978 |
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 B1B95/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.870 |
| C2 |
0.000 |
0.000 |
-1.070 |
| N3 |
0.000 |
0.000 |
0.115 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9401 | 1.7550 |
C2 | 2.9401 | | 1.1852 | N3 | 1.7550 | 1.1852 | |
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 B1B95/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.535 |
|
|
|
| 2 |
C |
0.089 |
|
|
|
| 3 |
N |
-0.624 |
|
|
|
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 |
8.340 |
8.340 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.142 |
0.000 |
0.000 |
| y |
0.000 |
-14.142 |
0.000 |
| z |
0.000 |
0.000 |
-2.664 |
|
| Traceless |
| | x | y | z |
| x |
-5.739 |
0.000 |
0.000 |
| y |
0.000 |
-5.739 |
0.000 |
| z |
0.000 |
0.000 |
11.478 |
|
| Polar |
| 3z2-r2 | 22.956 |
| 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 |
1.974 |
0.000 |
0.000 |
| y |
0.000 |
1.974 |
0.000 |
| z |
0.000 |
0.000 |
4.312 |
<r2> (average value of r
2) Å
2
| <r2> |
23.898 |
| (<r2>)1/2 |
4.889 |