Jump to
S1C2
S1C3
Energy calculated at B3LYP/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -692.831063 |
| Energy at 298.15K | -692.830436 |
| HF Energy | -692.831063 |
| Nuclear repulsion energy | 61.159814 |
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/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
0.000 |
1.306 |
| C2 |
0.000 |
0.000 |
-1.283 |
| N3 |
0.000 |
0.000 |
-2.446 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.5898 | 3.7527 |
C2 | 2.5898 | | 1.1630 | N3 | 3.7527 | 1.1630 | |
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/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.930 |
|
|
|
| 2 |
C |
-0.286 |
|
|
|
| 3 |
N |
-0.644 |
|
|
|
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 |
12.280 |
12.280 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.326 |
0.000 |
0.000 |
| y |
0.000 |
-23.326 |
0.000 |
| z |
0.000 |
0.000 |
-31.805 |
|
| Traceless |
| | x | y | z |
| x |
4.240 |
0.000 |
0.000 |
| y |
0.000 |
4.240 |
0.000 |
| z |
0.000 |
0.000 |
-8.479 |
|
| Polar |
| 3z2-r2 | -16.959 |
| 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 |
3.988 |
0.000 |
0.000 |
| y |
0.000 |
3.988 |
0.000 |
| z |
0.000 |
0.000 |
7.327 |
<r2> (average value of r
2) Å
2
| <r2> |
100.535 |
| (<r2>)1/2 |
10.027 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -692.834033 |
| Energy at 298.15K | |
| HF Energy | -692.834033 |
| Nuclear repulsion energy | 64.618606 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3LYP/6-311+G(3df,2p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
2135 |
2065 |
128.58 |
|
|
|
| 2 |
Σ |
311 |
301 |
85.06 |
|
|
|
| 3 |
Π |
35i |
34i |
1.27 |
|
|
|
| 3 |
Π |
35i |
34i |
1.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1188.2 cm
-1
Scaled (by 0.967) Zero Point Vibrational Energy (zpe) 1149.0 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3LYP/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
0.000 |
1.208 |
| C2 |
0.000 |
0.000 |
-2.397 |
| N3 |
0.000 |
0.000 |
-1.225 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 3.6055 | 2.4339 |
C2 | 3.6055 | | 1.1716 | N3 | 2.4339 | 1.1716 | |
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/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.935 |
|
|
|
| 2 |
C |
-0.178 |
|
|
|
| 3 |
N |
-0.757 |
|
|
|
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 |
12.091 |
12.091 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.283 |
0.000 |
0.000 |
| y |
0.000 |
-23.283 |
0.000 |
| z |
0.000 |
0.000 |
-33.600 |
|
| Traceless |
| | x | y | z |
| x |
5.159 |
0.000 |
0.000 |
| y |
0.000 |
5.159 |
0.000 |
| z |
0.000 |
0.000 |
-10.317 |
|
| Polar |
| 3z2-r2 | -20.634 |
| 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 |
4.014 |
0.000 |
0.000 |
| y |
0.000 |
4.014 |
0.000 |
| z |
0.000 |
0.000 |
7.094 |
<r2> (average value of r
2) Å
2
| <r2> |
89.425 |
| (<r2>)1/2 |
9.456 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -692.836781 |
| Energy at 298.15K | -692.836613 |
| HF Energy | -692.836781 |
| Nuclear repulsion energy | 68.605892 |
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/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
1.047 |
0.000 |
| C2 |
0.618 |
-1.653 |
0.000 |
| N3 |
-0.530 |
-1.424 |
0.000 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.7701 | 2.5274 |
C2 | 2.7701 | | 1.1709 | N3 | 2.5274 | 1.1709 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| K1 |
C2 |
N3 |
65.825 |
|
K1 |
N3 |
C2 |
89.172 |
| C2 |
K1 |
N3 |
25.003 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
K |
0.879 |
|
|
|
| 2 |
C |
-0.180 |
|
|
|
| 3 |
N |
-0.700 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.397 |
10.134 |
0.000 |
10.142 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.424 |
1.157 |
0.000 |
| y |
1.157 |
-26.757 |
0.000 |
| z |
0.000 |
0.000 |
-23.331 |
|
| Traceless |
| | x | y | z |
| x |
-2.379 |
1.157 |
0.000 |
| y |
1.157 |
-1.380 |
0.000 |
| z |
0.000 |
0.000 |
3.759 |
|
| Polar |
| 3z2-r2 | 7.518 |
| x2-y2 | -0.666 |
| xy | 1.157 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.097 |
-0.249 |
0.000 |
| y |
-0.249 |
5.534 |
0.000 |
| z |
0.000 |
0.000 |
4.073 |
<r2> (average value of r
2) Å
2
| <r2> |
71.822 |
| (<r2>)1/2 |
8.475 |