Jump to
S1C2
S2C1
S2C2
Energy calculated at B3LYP/6-31G**
| | hartrees |
| Energy at 0K | -131.423063 |
| Energy at 298.15K | -131.422370 |
| HF Energy | -131.423063 |
| Nuclear repulsion energy | 47.235472 |
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/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3400 |
3267 |
39.61 |
|
|
|
| 2 |
A' |
1799 |
1728 |
29.72 |
|
|
|
| 3 |
A' |
1249 |
1200 |
5.98 |
|
|
|
| 4 |
A' |
470 |
452 |
22.87 |
|
|
|
| 5 |
A' |
384 |
369 |
30.11 |
|
|
|
| 6 |
A" |
451 |
434 |
2.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3876.5 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 3724.6 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/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.077 |
-1.221 |
0.000 |
| C2 |
0.000 |
0.084 |
0.000 |
| N3 |
-0.155 |
1.281 |
0.000 |
| H4 |
0.621 |
-2.143 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3069 | 2.5121 | 1.0710 |
C2 | 1.3069 | | 1.2067 | 2.3122 | N3 | 2.5121 | 1.2067 | | 3.5108 | H4 | 1.0710 | 2.3122 | 3.5108 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.011 |
|
C2 |
C1 |
H4 |
152.882 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3LYP/6-31G**
| | hartrees |
| Energy at 0K | -131.422540 |
| Energy at 298.15K | |
| HF Energy | -131.422540 |
| Nuclear repulsion energy | 47.287575 |
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/6-31G**
| 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 |
3458 |
3323 |
71.45 |
|
|
|
| 2 |
Σ |
1748 |
1680 |
32.06 |
|
|
|
| 3 |
Σ |
1286 |
1235 |
4.03 |
|
|
|
| 4 |
Π |
453 |
436 |
1.03 |
|
|
|
| 4 |
Π |
453 |
436 |
1.03 |
|
|
|
| 5 |
Π |
277i |
266i |
49.57 |
|
|
|
| 5 |
Π |
277i |
266i |
49.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3421.9 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 3287.8 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/6-31G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.211 |
| C2 |
0.000 |
0.000 |
0.080 |
| N3 |
0.000 |
0.000 |
1.295 |
| H4 |
0.000 |
0.000 |
-2.277 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2905 | 2.5055 | 1.0662 |
C2 | 1.2905 | | 1.2150 | 2.3567 | N3 | 2.5055 | 1.2150 | | 3.5717 | H4 | 1.0662 | 2.3567 | 3.5717 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
180.000 |
|
C2 |
C1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.029 |
|
|
|
| 2 |
C |
0.302 |
|
|
|
| 3 |
N |
-0.472 |
|
|
|
| 4 |
H |
0.199 |
|
|
|
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 |
-3.246 |
3.246 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.856 |
0.000 |
0.000 |
| y |
0.000 |
-16.856 |
0.000 |
| z |
0.000 |
0.000 |
-15.270 |
|
| Traceless |
| | x | y | z |
| x |
-0.793 |
0.000 |
0.000 |
| y |
0.000 |
-0.793 |
0.000 |
| z |
0.000 |
0.000 |
1.586 |
|
| Polar |
| 3z2-r2 | 3.172 |
| 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 |
1.631 |
0.000 |
0.000 |
| y |
0.000 |
1.631 |
0.000 |
| z |
0.000 |
0.000 |
6.179 |
<r2> (average value of r
2) Å
2
| <r2> |
35.951 |
| (<r2>)1/2 |
5.996 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3LYP/6-31G**
| | hartrees |
| Energy at 0K | -131.396973 |
| Energy at 298.15K | -131.396415 |
| HF Energy | -131.396973 |
| Nuclear repulsion energy | 46.900081 |
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/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3072 |
2951 |
12.16 |
|
|
|
| 2 |
A' |
2104 |
2021 |
17.67 |
|
|
|
| 3 |
A' |
1096 |
1054 |
35.31 |
|
|
|
| 4 |
A' |
932 |
896 |
48.74 |
|
|
|
| 5 |
A' |
442 |
425 |
22.59 |
|
|
|
| 6 |
A" |
325 |
313 |
10.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3985.9 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 3829.6 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/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.117 |
-1.280 |
0.000 |
| C2 |
0.000 |
0.091 |
0.000 |
| N3 |
-0.268 |
1.246 |
0.000 |
| H4 |
1.174 |
-1.591 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3760 | 2.5543 | 1.1012 |
C2 | 1.3760 | | 1.1848 | 2.0509 | N3 | 2.5543 | 1.1848 | | 3.1815 | H4 | 1.1012 | 2.0509 | 3.1815 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.076 |
|
|
|
| 2 |
C |
0.323 |
|
|
|
| 3 |
N |
-0.404 |
|
|
|
| 4 |
H |
0.157 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.771 |
-1.344 |
0.000 |
2.223 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.525 |
-2.152 |
0.000 |
| y |
-2.152 |
-20.839 |
0.000 |
| z |
0.000 |
0.000 |
-15.524 |
|
| Traceless |
| | x | y | z |
| x |
1.656 |
-2.152 |
0.000 |
| y |
-2.152 |
-4.815 |
0.000 |
| z |
0.000 |
0.000 |
3.158 |
|
| Polar |
| 3z2-r2 | 6.317 |
| x2-y2 | 4.314 |
| xy | -2.152 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.449 |
-0.907 |
0.000 |
| y |
-0.907 |
6.030 |
0.000 |
| z |
0.000 |
0.000 |
2.177 |
<r2> (average value of r
2) Å
2
| <r2> |
36.237 |
| (<r2>)1/2 |
6.020 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3LYP/6-31G**
| | hartrees |
| Energy at 0K | -131.396973 |
| Energy at 298.15K | -131.396415 |
| HF Energy | -131.396973 |
| Nuclear repulsion energy | 46.900081 |
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/6-31G**
Geometric Data calculated at B3LYP/6-31G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability