Jump to
S1C2
S1C3
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -692.848250 |
| Energy at 298.15K | -692.847664 |
| HF Energy | -692.848250 |
| Nuclear repulsion energy | 60.163752 |
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/TZVP
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
0.000 |
1.337 |
| C2 |
0.000 |
0.000 |
-1.328 |
| N3 |
0.000 |
0.000 |
-2.490 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.6651 | 3.8266 |
C2 | 2.6651 | | 1.1614 | N3 | 3.8266 | 1.1614 | |
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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.918 |
|
|
|
| 2 |
C |
-0.627 |
|
|
|
| 3 |
N |
-0.292 |
|
|
|
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 |
13.272 |
13.272 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.091 |
0.000 |
0.000 |
| y |
0.000 |
-23.091 |
0.000 |
| z |
0.000 |
0.000 |
-30.536 |
|
| Traceless |
| | x | y | z |
| x |
3.722 |
0.000 |
0.000 |
| y |
0.000 |
3.722 |
0.000 |
| z |
0.000 |
0.000 |
-7.444 |
|
| Polar |
| 3z2-r2 | -14.889 |
| 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 |
2.760 |
0.000 |
0.000 |
| y |
0.000 |
2.760 |
0.000 |
| z |
0.000 |
0.000 |
5.993 |
<r2> (average value of r
2) Å
2
| <r2> |
103.906 |
| (<r2>)1/2 |
10.193 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -692.850850 |
| Energy at 298.15K | -692.850249 |
| HF Energy | -692.850850 |
| Nuclear repulsion energy | 63.361859 |
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/TZVP
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
0.000 |
1.241 |
| C2 |
0.000 |
0.000 |
-2.443 |
| N3 |
0.000 |
0.000 |
-1.274 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 3.6846 | 2.5155 |
C2 | 3.6846 | | 1.1691 | N3 | 2.5155 | 1.1691 | |
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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.925 |
|
|
|
| 2 |
C |
-0.398 |
|
|
|
| 3 |
N |
-0.527 |
|
|
|
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 |
13.274 |
13.274 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.951 |
0.000 |
0.000 |
| y |
0.000 |
-22.951 |
0.000 |
| z |
0.000 |
0.000 |
-33.015 |
|
| Traceless |
| | x | y | z |
| x |
5.032 |
0.000 |
0.000 |
| y |
0.000 |
5.032 |
0.000 |
| z |
0.000 |
0.000 |
-10.064 |
|
| Polar |
| 3z2-r2 | -20.127 |
| 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 |
2.618 |
0.000 |
0.000 |
| y |
0.000 |
2.618 |
0.000 |
| z |
0.000 |
0.000 |
5.667 |
<r2> (average value of r
2) Å
2
| <r2> |
92.890 |
| (<r2>)1/2 |
9.638 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/TZVP
| | hartrees |
| Energy at 0K | -692.852581 |
| Energy at 298.15K | -692.852355 |
| HF Energy | -692.852581 |
| Nuclear repulsion energy | 67.153879 |
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/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
1.079 |
0.000 |
| C2 |
0.626 |
-1.641 |
0.000 |
| N3 |
-0.536 |
-1.521 |
0.000 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.7910 | 2.6540 |
C2 | 2.7910 | | 1.1685 | N3 | 2.6540 | 1.1685 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| K1 |
C2 |
N3 |
71.112 |
|
K1 |
N3 |
C2 |
84.269 |
| C2 |
K1 |
N3 |
24.618 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.864 |
|
|
|
| 2 |
C |
-0.445 |
|
|
|
| 3 |
N |
-0.419 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.413 |
11.366 |
0.000 |
11.374 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.556 |
0.787 |
0.000 |
| y |
0.787 |
-26.522 |
0.000 |
| z |
0.000 |
0.000 |
-23.218 |
|
| Traceless |
| | x | y | z |
| x |
-2.686 |
0.787 |
0.000 |
| y |
0.787 |
-1.135 |
0.000 |
| z |
0.000 |
0.000 |
3.821 |
|
| Polar |
| 3z2-r2 | 7.643 |
| x2-y2 | -1.034 |
| xy | 0.787 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.350 |
-0.188 |
0.000 |
| y |
-0.188 |
3.744 |
0.000 |
| z |
0.000 |
0.000 |
2.895 |
<r2> (average value of r
2) Å
2
| <r2> |
74.911 |
| (<r2>)1/2 |
8.655 |