Jump to
S1C2
S1C3
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -120.973447 |
| Energy at 298.15K | -120.972904 |
| HF Energy | -120.973447 |
| Nuclear repulsion energy | 38.121172 |
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/LANL2DZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
0.000 |
1.331 |
| C2 |
0.000 |
0.000 |
-1.300 |
| N3 |
0.000 |
0.000 |
-2.498 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.6303 | 3.8285 |
C2 | 2.6303 | | 1.1982 | N3 | 3.8285 | 1.1982 | |
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 B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.767 |
|
|
|
| 2 |
C |
-0.566 |
|
|
|
| 3 |
N |
-0.200 |
|
|
|
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 |
12.963 |
12.963 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.049 |
0.000 |
0.000 |
| y |
0.000 |
-23.049 |
0.000 |
| z |
0.000 |
0.000 |
-29.986 |
|
| Traceless |
| | x | y | z |
| x |
3.469 |
0.000 |
0.000 |
| y |
0.000 |
3.469 |
0.000 |
| z |
0.000 |
0.000 |
-6.937 |
|
| Polar |
| 3z2-r2 | -13.874 |
| 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 |
3.049 |
0.000 |
0.000 |
| y |
0.000 |
3.049 |
0.000 |
| z |
0.000 |
0.000 |
6.103 |
<r2> (average value of r
2) Å
2
| <r2> |
85.584 |
| (<r2>)1/2 |
9.251 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -120.975345 |
| Energy at 298.15K | -120.974745 |
| HF Energy | -120.975345 |
| Nuclear repulsion energy | 39.600585 |
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/LANL2DZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
0.000 |
1.234 |
| C2 |
0.000 |
0.000 |
-2.454 |
| N3 |
0.000 |
0.000 |
-1.247 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 3.6884 | 2.4818 |
C2 | 3.6884 | | 1.2066 | N3 | 2.4818 | 1.2066 | |
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 B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.782 |
|
|
|
| 2 |
C |
-0.288 |
|
|
|
| 3 |
N |
-0.494 |
|
|
|
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 |
12.905 |
12.905 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.850 |
0.000 |
0.000 |
| y |
0.000 |
-22.850 |
0.000 |
| z |
0.000 |
0.000 |
-32.549 |
|
| Traceless |
| | x | y | z |
| x |
4.850 |
0.000 |
0.000 |
| y |
0.000 |
4.850 |
0.000 |
| z |
0.000 |
0.000 |
-9.700 |
|
| Polar |
| 3z2-r2 | -19.400 |
| 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 |
2.836 |
0.000 |
-0.000 |
| y |
0.000 |
2.836 |
0.000 |
| z |
-0.000 |
0.000 |
6.102 |
<r2> (average value of r
2) Å
2
| <r2> |
77.027 |
| (<r2>)1/2 |
8.777 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -120.973950 |
| Energy at 298.15K | -120.973659 |
| HF Energy | -120.973950 |
| Nuclear repulsion energy | 41.048717 |
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/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
1.092 |
0.000 |
| C2 |
0.621 |
-1.786 |
0.000 |
| N3 |
-0.532 |
-1.431 |
0.000 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.9442 | 2.5786 |
C2 | 2.9442 | | 1.2070 | N3 | 2.5786 | 1.2070 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| K1 |
C2 |
N3 |
60.718 |
|
K1 |
N3 |
C2 |
95.186 |
| C2 |
K1 |
N3 |
24.096 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.726 |
|
|
|
| 2 |
C |
-0.319 |
|
|
|
| 3 |
N |
-0.407 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.284 |
11.467 |
0.000 |
11.471 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.753 |
1.583 |
0.000 |
| y |
1.583 |
-26.599 |
0.000 |
| z |
0.000 |
0.000 |
-23.228 |
|
| Traceless |
| | x | y | z |
| x |
-2.840 |
1.583 |
0.000 |
| y |
1.583 |
-1.108 |
0.000 |
| z |
0.000 |
0.000 |
3.948 |
|
| Polar |
| 3z2-r2 | 7.896 |
| x2-y2 | -1.154 |
| xy | 1.583 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.479 |
-0.374 |
0.000 |
| y |
-0.374 |
3.784 |
0.000 |
| z |
0.000 |
0.000 |
3.164 |
<r2> (average value of r
2) Å
2
| <r2> |
64.666 |
| (<r2>)1/2 |
8.042 |