Jump to
S1C2
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -120.141162 |
Energy at 298.15K | -120.140637 |
HF Energy | -120.141162 |
Nuclear repulsion energy | 38.229429 |
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/LANL2DZ
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
K1 |
0.000 |
0.000 |
1.347 |
C2 |
0.000 |
0.000 |
-1.336 |
N3 |
0.000 |
0.000 |
-2.510 |
Atom - Atom Distances (Å)
|
K1 |
C2 |
N3 |
K1 | | 2.6824 | 3.8564 |
C2 | 2.6824 | | 1.1740 | N3 | 3.8564 | 1.1740 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
K1 |
C2 |
N3 |
180.000 |
|
K1 |
N3 |
C2 |
0.000 |
C2 |
K1 |
N3 |
0.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
K |
0.855 |
|
|
|
2 |
C |
-0.577 |
|
|
|
3 |
N |
-0.278 |
|
|
|
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 |
13.952 |
13.952 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.601 |
0.000 |
0.000 |
y |
0.000 |
-22.601 |
0.000 |
z |
0.000 |
0.000 |
-31.579 |
|
Traceless |
| x | y | z |
x |
4.489 |
0.000 |
0.000 |
y |
0.000 |
4.489 |
0.000 |
z |
0.000 |
0.000 |
-8.978 |
|
Polar |
3z2-r2 | -17.955 |
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 |
2.054 |
0.000 |
0.000 |
y |
0.000 |
2.054 |
0.000 |
z |
0.000 |
0.000 |
4.318 |
<r2> (average value of r
2) Å
2
<r2> |
87.107 |
(<r2>)1/2 |
9.333 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -120.149811 |
Energy at 298.15K | -120.149343 |
HF Energy | -120.149811 |
Nuclear repulsion energy | 39.906168 |
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/LANL2DZ
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
K1 |
0.000 |
0.000 |
1.235 |
C2 |
0.000 |
0.000 |
-2.443 |
N3 |
0.000 |
0.000 |
-1.259 |
Atom - Atom Distances (Å)
|
K1 |
C2 |
N3 |
K1 | | 3.6781 | 2.4939 |
C2 | 3.6781 | | 1.1841 | N3 | 2.4939 | 1.1841 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
K1 |
C2 |
N3 |
0.000 |
|
K1 |
N3 |
C2 |
180.000 |
C2 |
K1 |
N3 |
0.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
K |
0.872 |
|
|
|
2 |
C |
-0.241 |
|
|
|
3 |
N |
-0.631 |
|
|
|
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 |
13.075 |
13.075 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.326 |
0.000 |
0.000 |
y |
0.000 |
-22.326 |
0.000 |
z |
0.000 |
0.000 |
-31.895 |
|
Traceless |
| x | y | z |
x |
4.784 |
0.000 |
0.000 |
y |
0.000 |
4.784 |
0.000 |
z |
0.000 |
0.000 |
-9.568 |
|
Polar |
3z2-r2 | -19.137 |
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 |
1.908 |
0.000 |
0.000 |
y |
0.000 |
1.908 |
0.000 |
z |
0.000 |
0.000 |
4.107 |
<r2> (average value of r
2) Å
2
<r2> |
76.565 |
(<r2>)1/2 |
8.750 |