Jump to
S2C1
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -145.569767 |
| Energy at 298.15K | -145.569247 |
| HF Energy | -145.569767 |
| Nuclear repulsion energy | 44.448844 |
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/STO-3G
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.000 |
| N2 |
0.000 |
0.000 |
1.292 |
| N3 |
0.000 |
0.000 |
-1.292 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
N3 |
| C1 | | 1.2917 | 1.2917 |
N2 | 1.2917 | | 2.5835 | N3 | 1.2917 | 2.5835 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N2 |
C1 |
N3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.112 |
|
|
|
| 2 |
N |
-0.056 |
|
|
|
| 3 |
N |
-0.056 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.122 |
0.000 |
0.000 |
| y |
0.000 |
-14.122 |
0.000 |
| z |
0.000 |
0.000 |
-18.788 |
|
| Traceless |
| | x | y | z |
| x |
2.333 |
0.000 |
0.000 |
| y |
0.000 |
2.333 |
0.000 |
| z |
0.000 |
0.000 |
-4.666 |
|
| Polar |
| 3z2-r2 | -9.332 |
| 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 |
0.749 |
0.000 |
0.000 |
| y |
0.000 |
0.749 |
0.000 |
| z |
0.000 |
0.000 |
3.157 |
<r2> (average value of r
2) Å
2
| <r2> |
33.152 |
| (<r2>)1/2 |
5.758 |
Jump to
S1C1
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -145.504274 |
| Energy at 298.15K | -145.503810 |
| HF Energy | -145.504274 |
| Nuclear repulsion energy | 44.701945 |
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/STO-3G
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.000 |
| N2 |
0.000 |
0.000 |
1.284 |
| N3 |
0.000 |
0.000 |
-1.284 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
N3 |
| C1 | | 1.2844 | 1.2844 |
N2 | 1.2844 | | 2.5688 | N3 | 1.2844 | 2.5688 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N2 |
C1 |
N3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.116 |
|
|
|
| 2 |
N |
-0.058 |
|
|
|
| 3 |
N |
-0.058 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.175 |
0.000 |
0.000 |
| y |
0.000 |
-13.083 |
0.000 |
| z |
0.000 |
0.000 |
-18.767 |
|
| Traceless |
| | x | y | z |
| x |
0.750 |
0.000 |
0.000 |
| y |
0.000 |
3.888 |
0.000 |
| z |
0.000 |
0.000 |
-4.637 |
|
| Polar |
| 3z2-r2 | -9.275 |
| x2-y2 | -2.092 |
| 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 |
0.445 |
0.000 |
0.000 |
| y |
0.000 |
0.891 |
0.000 |
| z |
0.000 |
0.000 |
3.329 |
<r2> (average value of r
2) Å
2
| <r2> |
32.886 |
| (<r2>)1/2 |
5.735 |