Jump to
S1C2
S1C3
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.380621 |
| Energy at 298.15K | -100.379619 |
| HF Energy | -100.380621 |
| Nuclear repulsion energy | 27.709375 |
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 B3LYP/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.052 |
| C2 |
0.000 |
0.000 |
-0.154 |
| N3 |
0.000 |
0.000 |
1.012 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.8972 | 3.0632 |
C2 | 1.8972 | | 1.1660 | N3 | 3.0632 | 1.1660 | |
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 B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.166 |
|
|
|
| 2 |
C |
0.166 |
|
|
|
| 3 |
N |
-0.332 |
|
|
|
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 |
-8.673 |
8.673 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.190 |
0.000 |
0.000 |
| y |
0.000 |
-14.190 |
0.000 |
| z |
0.000 |
0.000 |
1.315 |
|
| Traceless |
| | x | y | z |
| x |
-7.753 |
0.000 |
0.000 |
| y |
0.000 |
-7.753 |
0.000 |
| z |
0.000 |
0.000 |
15.506 |
|
| Polar |
| 3z2-r2 | 31.011 |
| 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 |
2.768 |
0.000 |
0.000 |
| y |
0.000 |
2.768 |
0.000 |
| z |
0.000 |
0.000 |
4.308 |
<r2> (average value of r
2) Å
2
| <r2> |
25.569 |
| (<r2>)1/2 |
5.057 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.388239 |
| Energy at 298.15K | -100.387482 |
| HF Energy | -100.388239 |
| Nuclear repulsion energy | 29.276345 |
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 B3LYP/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.439 |
-0.575 |
0.000 |
| C2 |
-0.720 |
-0.370 |
0.000 |
| N3 |
0.000 |
0.564 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1686 | 1.8352 |
C2 | 2.1686 | | 1.1792 | N3 | 1.8352 | 1.1792 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
57.799 |
|
Li1 |
N3 |
C2 |
89.264 |
| C2 |
Li1 |
N3 |
32.937 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.176 |
|
|
|
| 2 |
C |
-0.004 |
|
|
|
| 3 |
N |
-0.172 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.368 |
-2.235 |
0.000 |
6.749 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-5.632 |
-5.735 |
0.000 |
| y |
-5.735 |
-15.325 |
0.000 |
| z |
0.000 |
0.000 |
-14.560 |
|
| Traceless |
| | x | y | z |
| x |
9.311 |
-5.735 |
0.000 |
| y |
-5.735 |
-5.230 |
0.000 |
| z |
0.000 |
0.000 |
-4.081 |
|
| Polar |
| 3z2-r2 | -8.162 |
| x2-y2 | 9.693 |
| xy | -5.735 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.448 |
0.380 |
0.000 |
| y |
0.380 |
3.427 |
0.000 |
| z |
0.000 |
0.000 |
2.870 |
<r2> (average value of r
2) Å
2
| <r2> |
20.802 |
| (<r2>)1/2 |
4.561 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.388130 |
| Energy at 298.15K | -100.387062 |
| HF Energy | -100.388130 |
| Nuclear repulsion energy | 28.439217 |
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 B3LYP/6-31G(2df,p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
2148 |
2073 |
166.79 |
|
|
|
| 2 |
Σ |
745 |
719 |
134.23 |
|
|
|
| 3 |
Π |
115 |
111 |
25.01 |
|
|
|
| 3 |
Π |
115 |
111 |
25.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1561.2 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 1506.6 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3LYP/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.867 |
| C2 |
0.000 |
0.000 |
-1.066 |
| N3 |
0.000 |
0.000 |
0.113 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9329 | 1.7543 |
C2 | 2.9329 | | 1.1786 | N3 | 1.7543 | 1.1786 | |
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 B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.315 |
|
|
|
| 2 |
C |
-0.291 |
|
|
|
| 3 |
N |
-0.024 |
|
|
|
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 |
8.465 |
8.465 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.255 |
0.000 |
0.000 |
| y |
0.000 |
-14.255 |
0.000 |
| z |
0.000 |
0.000 |
-2.036 |
|
| Traceless |
| | x | y | z |
| x |
-6.109 |
0.000 |
0.000 |
| y |
0.000 |
-6.109 |
0.000 |
| z |
0.000 |
0.000 |
12.219 |
|
| Polar |
| 3z2-r2 | 24.437 |
| 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 |
2.733 |
0.000 |
0.000 |
| y |
0.000 |
2.733 |
0.000 |
| z |
0.000 |
0.000 |
4.333 |
<r2> (average value of r
2) Å
2
| <r2> |
23.723 |
| (<r2>)1/2 |
4.871 |