Jump to
S1C2
S1C3
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -692.780034 |
Energy at 298.15K | -692.779416 |
HF Energy | -692.780034 |
Nuclear repulsion energy | 60.798295 |
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 B1B95/6-31G*
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
K1 |
0.000 |
0.000 |
1.314 |
C2 |
0.000 |
0.000 |
-1.291 |
N3 |
0.000 |
0.000 |
-2.461 |
Atom - Atom Distances (Å)
|
K1 |
C2 |
N3 |
K1 | | 2.6052 | 3.7750 |
C2 | 2.6052 | | 1.1699 | N3 | 3.7750 | 1.1699 | |
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 B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
K |
0.682 |
|
|
|
2 |
C |
-0.247 |
|
|
|
3 |
N |
-0.435 |
|
|
|
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 |
12.123 |
12.123 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.905 |
0.000 |
0.000 |
y |
0.000 |
-22.905 |
0.000 |
z |
0.000 |
0.000 |
-30.113 |
|
Traceless |
| x | y | z |
x |
3.604 |
0.000 |
0.000 |
y |
0.000 |
3.604 |
0.000 |
z |
0.000 |
0.000 |
-7.207 |
|
Polar |
3z2-r2 | -14.415 |
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 |
3.082 |
0.000 |
-0.000 |
y |
0.000 |
3.082 |
-0.000 |
z |
-0.000 |
-0.000 |
6.017 |
<r2> (average value of r
2) Å
2
<r2> |
101.012 |
(<r2>)1/2 |
10.050 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -692.780495 |
Energy at 298.15K | |
HF Energy | -692.780495 |
Nuclear repulsion energy | 64.110349 |
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 B1B95/6-31G*
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
K1 |
0.000 |
0.000 |
1.219 |
C2 |
0.000 |
0.000 |
-2.416 |
N3 |
0.000 |
0.000 |
-1.237 |
Atom - Atom Distances (Å)
|
K1 |
C2 |
N3 |
K1 | | 3.6346 | 2.4559 |
C2 | 3.6346 | | 1.1788 | N3 | 2.4559 | 1.1788 | |
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 B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
K |
0.723 |
|
|
|
2 |
C |
-0.136 |
|
|
|
3 |
N |
-0.587 |
|
|
|
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 |
11.995 |
11.995 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.910 |
0.000 |
0.000 |
y |
0.000 |
-22.910 |
0.000 |
z |
0.000 |
0.000 |
-31.999 |
|
Traceless |
| x | y | z |
x |
4.545 |
0.000 |
0.000 |
y |
0.000 |
4.545 |
0.000 |
z |
0.000 |
0.000 |
-9.089 |
|
Polar |
3z2-r2 | -18.178 |
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 |
2.958 |
-0.001 |
0.025 |
y |
-0.001 |
2.958 |
0.033 |
z |
0.025 |
0.033 |
5.311 |
<r2> (average value of r
2) Å
2
<r2> |
90.155 |
(<r2>)1/2 |
9.495 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -692.788033 |
Energy at 298.15K | -692.787945 |
HF Energy | -692.788033 |
Nuclear repulsion energy | 68.684019 |
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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
K1 |
0.000 |
1.039 |
0.000 |
C2 |
0.632 |
-1.576 |
0.000 |
N3 |
-0.542 |
-1.470 |
0.000 |
Atom - Atom Distances (Å)
|
K1 |
C2 |
N3 |
K1 | | 2.6910 | 2.5676 |
C2 | 2.6910 | | 1.1787 | N3 | 2.5676 | 1.1787 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
K1 |
C2 |
N3 |
71.261 |
|
K1 |
N3 |
C2 |
82.971 |
C2 |
K1 |
N3 |
25.769 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
K |
0.649 |
|
|
|
2 |
C |
-0.159 |
|
|
|
3 |
N |
-0.491 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.394 |
9.957 |
0.000 |
9.965 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-27.143 |
0.557 |
0.000 |
y |
0.557 |
-25.721 |
0.000 |
z |
0.000 |
0.000 |
-23.151 |
|
Traceless |
| x | y | z |
x |
-2.707 |
0.557 |
0.000 |
y |
0.557 |
-0.574 |
0.000 |
z |
0.000 |
0.000 |
3.280 |
|
Polar |
3z2-r2 | 6.560 |
x2-y2 | -1.422 |
xy | 0.557 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.422 |
-0.057 |
0.000 |
y |
-0.057 |
4.346 |
0.000 |
z |
0.000 |
0.000 |
3.321 |
<r2> (average value of r
2) Å
2
<r2> |
70.848 |
(<r2>)1/2 |
8.417 |