Jump to
S1C2
S1C3
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -689.287044 |
| Energy at 298.15K | -689.286323 |
| HF Energy | -689.287044 |
| Nuclear repulsion energy | 60.946672 |
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) |
| K1 |
0.000 |
0.000 |
1.308 |
| C2 |
0.000 |
0.000 |
-1.279 |
| N3 |
0.000 |
0.000 |
-2.454 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.5864 | 3.7616 |
C2 | 2.5864 | | 1.1752 | N3 | 3.7616 | 1.1752 | |
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 B1B95/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.584 |
|
|
|
| 2 |
C |
-0.116 |
|
|
|
| 3 |
N |
-0.468 |
|
|
|
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 |
12.096 |
12.096 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.472 |
0.000 |
0.000 |
| y |
0.000 |
-23.472 |
0.000 |
| z |
0.000 |
0.000 |
-29.168 |
|
| Traceless |
| | x | y | z |
| x |
2.848 |
0.000 |
0.000 |
| y |
0.000 |
2.848 |
0.000 |
| z |
0.000 |
0.000 |
-5.696 |
|
| Polar |
| 3z2-r2 | -11.393 |
| 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 |
3.215 |
0.000 |
0.000 |
| y |
0.000 |
3.215 |
0.000 |
| z |
0.000 |
0.000 |
5.449 |
<r2> (average value of r
2) Å
2
| <r2> |
100.299 |
| (<r2>)1/2 |
10.015 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -689.294039 |
| Energy at 298.15K | |
| HF Energy | -689.294039 |
| Nuclear repulsion energy | 64.556239 |
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) |
| K1 |
0.000 |
0.000 |
1.205 |
| C2 |
0.000 |
0.000 |
-2.400 |
| N3 |
0.000 |
0.000 |
-1.215 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 3.6058 | 2.4201 |
C2 | 3.6058 | | 1.1857 | N3 | 2.4201 | 1.1857 | |
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 B1B95/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.563 |
|
|
|
| 2 |
C |
-0.001 |
|
|
|
| 3 |
N |
-0.562 |
|
|
|
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 |
12.008 |
12.008 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.468 |
0.000 |
0.000 |
| y |
0.000 |
-23.468 |
0.000 |
| z |
0.000 |
0.000 |
-31.490 |
|
| Traceless |
| | x | y | z |
| x |
4.011 |
0.000 |
0.000 |
| y |
0.000 |
4.011 |
0.000 |
| z |
0.000 |
0.000 |
-8.022 |
|
| Polar |
| 3z2-r2 | -16.044 |
| 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 |
3.080 |
0.000 |
0.000 |
| y |
0.000 |
3.080 |
0.000 |
| z |
0.000 |
0.000 |
5.433 |
<r2> (average value of r
2) Å
2
| <r2> |
88.836 |
| (<r2>)1/2 |
9.425 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -689.298116 |
| Energy at 298.15K | -689.297938 |
| HF Energy | -689.298116 |
| Nuclear repulsion energy | 68.314419 |
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 Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
1.047 |
0.000 |
| C2 |
0.625 |
-1.663 |
0.000 |
| N3 |
-0.536 |
-1.417 |
0.000 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.7818 | 2.5225 |
C2 | 2.7818 | | 1.1868 | N3 | 2.5225 | 1.1868 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| K1 |
C2 |
N3 |
65.063 |
|
K1 |
N3 |
C2 |
89.683 |
| C2 |
K1 |
N3 |
25.254 |
|
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 |
K |
0.504 |
|
|
|
| 2 |
C |
-0.021 |
|
|
|
| 3 |
N |
-0.482 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.352 |
10.270 |
0.000 |
10.276 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.963 |
1.126 |
0.000 |
| y |
1.126 |
-25.580 |
0.000 |
| z |
0.000 |
0.000 |
-23.719 |
|
| Traceless |
| | x | y | z |
| x |
-3.314 |
1.126 |
0.000 |
| y |
1.126 |
0.261 |
0.000 |
| z |
0.000 |
0.000 |
3.053 |
|
| Polar |
| 3z2-r2 | 6.106 |
| x2-y2 | -2.383 |
| xy | 1.126 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.190 |
-0.217 |
0.000 |
| y |
-0.217 |
3.714 |
0.000 |
| z |
0.000 |
0.000 |
3.099 |
<r2> (average value of r
2) Å
2
| <r2> |
71.948 |
| (<r2>)1/2 |
8.482 |