Jump to
S1C2
S2C1
S2C2
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -131.426197 |
| Energy at 298.15K | -131.425363 |
| HF Energy | -131.426197 |
| Nuclear repulsion energy | 47.151379 |
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 BLYP/6-311G**
| 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' |
3333 |
3320 |
46.68 |
|
|
|
| 2 |
A' |
1757 |
1751 |
20.82 |
|
|
|
| 3 |
A' |
1223 |
1219 |
2.95 |
|
|
|
| 4 |
A' |
442 |
441 |
3.47 |
|
|
|
| 5 |
A' |
281 |
280 |
51.84 |
|
|
|
| 6 |
A" |
443 |
442 |
0.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3740.1 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 3725.5 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.085 |
-1.217 |
0.000 |
| C2 |
0.000 |
0.081 |
0.000 |
| N3 |
-0.148 |
1.287 |
0.000 |
| H4 |
0.528 |
-2.194 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3006 | 2.5142 | 1.0725 |
C2 | 1.3006 | | 1.2145 | 2.3353 | N3 | 2.5142 | 1.2145 | | 3.5454 | H4 | 1.0725 | 2.3353 | 3.5454 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.738 |
|
C2 |
C1 |
H4 |
159.406 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -131.426058 |
| Energy at 298.15K | |
| HF Energy | -131.426058 |
| Nuclear repulsion energy | 47.185322 |
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 BLYP/6-311G**
| 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 |
3373 |
3360 |
67.18 |
|
|
|
| 2 |
Σ |
1739 |
1733 |
20.29 |
|
|
|
| 3 |
Σ |
1240 |
1235 |
2.41 |
|
|
|
| 4 |
Π |
445 |
443 |
0.59 |
|
|
|
| 4 |
Π |
445 |
443 |
0.59 |
|
|
|
| 5 |
Π |
182i |
181i |
48.96 |
|
|
|
| 5 |
Π |
182i |
181i |
48.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3439.0 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 3425.6 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 BLYP/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.213 |
| C2 |
0.000 |
0.000 |
0.079 |
| N3 |
0.000 |
0.000 |
1.298 |
| H4 |
0.000 |
0.000 |
-2.282 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2917 | 2.5105 | 1.0693 |
C2 | 1.2917 | | 1.2188 | 2.3610 | N3 | 2.5105 | 1.2188 | | 3.5798 | H4 | 1.0693 | 2.3610 | 3.5798 | |
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 BLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.029 |
|
|
|
| 2 |
C |
-0.009 |
|
|
|
| 3 |
N |
-0.178 |
|
|
|
| 4 |
H |
0.158 |
|
|
|
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 |
-3.134 |
3.134 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.273 |
0.000 |
0.000 |
| y |
0.000 |
-17.273 |
0.000 |
| z |
0.000 |
0.000 |
-15.672 |
|
| Traceless |
| | x | y | z |
| x |
-0.800 |
0.000 |
0.000 |
| y |
0.000 |
-0.800 |
0.000 |
| z |
0.000 |
0.000 |
1.601 |
|
| Polar |
| 3z2-r2 | 3.201 |
| 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 |
1.944 |
0.000 |
0.000 |
| y |
0.000 |
1.944 |
0.000 |
| z |
0.000 |
0.000 |
6.537 |
<r2> (average value of r
2) Å
2
| <r2> |
36.314 |
| (<r2>)1/2 |
6.026 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -131.404244 |
| Energy at 298.15K | -131.403676 |
| HF Energy | -131.404244 |
| Nuclear repulsion energy | 46.759118 |
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 BLYP/6-311G**
| 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' |
2979 |
2967 |
10.93 |
|
|
|
| 2 |
A' |
2000 |
1992 |
16.24 |
|
|
|
| 3 |
A' |
1076 |
1072 |
25.46 |
|
|
|
| 4 |
A' |
904 |
900 |
56.74 |
|
|
|
| 5 |
A' |
451 |
449 |
20.96 |
|
|
|
| 6 |
A" |
313 |
311 |
8.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3860.8 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 3845.8 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.229 |
-1.263 |
0.000 |
| C2 |
0.000 |
0.090 |
0.000 |
| N3 |
-0.383 |
1.220 |
0.000 |
| H4 |
1.308 |
-1.505 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3726 | 2.5577 | 1.1061 |
C2 | 1.3726 | | 1.1933 | 2.0632 | N3 | 2.5577 | 1.1933 | | 3.2076 | H4 | 1.1061 | 2.0632 | 3.2076 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.054 |
|
|
|
| 2 |
C |
0.059 |
|
|
|
| 3 |
N |
-0.160 |
|
|
|
| 4 |
H |
0.155 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.839 |
-1.102 |
0.000 |
2.144 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.601 |
-1.793 |
0.000 |
| y |
-1.793 |
-21.468 |
0.000 |
| z |
0.000 |
0.000 |
-15.874 |
|
| Traceless |
| | x | y | z |
| x |
2.070 |
-1.793 |
0.000 |
| y |
-1.793 |
-5.230 |
0.000 |
| z |
0.000 |
0.000 |
3.160 |
|
| Polar |
| 3z2-r2 | 6.319 |
| x2-y2 | 4.867 |
| xy | -1.793 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.909 |
-1.155 |
0.000 |
| y |
-1.155 |
6.290 |
0.000 |
| z |
0.000 |
0.000 |
2.407 |
<r2> (average value of r
2) Å
2
| <r2> |
36.595 |
| (<r2>)1/2 |
6.049 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -131.404244 |
| Energy at 298.15K | -131.403676 |
| HF Energy | -131.404244 |
| Nuclear repulsion energy | 46.759118 |
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 BLYP/6-311G**
Geometric Data calculated at BLYP/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability