Jump to
S1C2
S2C1
S2C2
Energy calculated at G4
| | hartrees |
| Energy at 0K | -131.364178 |
| Energy at 298.15K | -131.359469 |
| HF Energy | -131.429250 |
| Nuclear repulsion energy | 47.449930 |
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(2df,p)
| 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' |
3420 |
3300 |
49.25 |
|
|
|
| 2 |
A' |
1777 |
1715 |
36.34 |
|
|
|
| 3 |
A' |
1258 |
1214 |
5.60 |
|
|
|
| 4 |
A' |
460 |
444 |
5.81 |
|
|
|
| 5 |
A' |
321 |
309 |
46.38 |
|
|
|
| 6 |
A" |
461 |
445 |
1.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3848.3 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3713.6 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(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.084 |
-1.211 |
0.000 |
| C2 |
0.000 |
0.082 |
0.000 |
| N3 |
-0.151 |
1.277 |
0.000 |
| H4 |
0.553 |
-2.169 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2953 | 2.4989 | 1.0671 |
C2 | 1.2953 | | 1.2047 | 2.3179 | N3 | 2.4989 | 1.2047 | | 3.5174 | H4 | 1.0671 | 2.3179 | 3.5174 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
177.650 |
|
C2 |
C1 |
H4 |
145.377 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at G4
| | hartrees |
| Energy at 0K | -131.363886 |
| Energy at 298.15K | -131.360048 |
| HF Energy | -131.429012 |
| Nuclear repulsion energy | 47.486630 |
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(2df,p)
| 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 |
3467 |
3346 |
72.26 |
|
|
|
| 2 |
Σ |
1744 |
1683 |
38.03 |
|
|
|
| 3 |
Σ |
1283 |
1238 |
3.76 |
|
|
|
| 4 |
Π |
462 |
446 |
0.68 |
|
|
|
| 4 |
Π |
462 |
446 |
0.68 |
|
|
|
| 5 |
Π |
232i |
224i |
46.89 |
|
|
|
| 5 |
Π |
232i |
224i |
46.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3476.4 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3354.7 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(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.205 |
| C2 |
0.000 |
0.000 |
0.079 |
| N3 |
0.000 |
0.000 |
1.289 |
| H4 |
0.000 |
0.000 |
-2.268 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2835 | 2.4942 | 1.0634 |
C2 | 1.2835 | | 1.2108 | 2.3469 | N3 | 2.4942 | 1.2108 | | 3.5576 | H4 | 1.0634 | 2.3469 | 3.5576 | |
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(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.185 |
|
|
|
| 2 |
C |
0.271 |
|
|
|
| 3 |
N |
-0.324 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
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 |
-3.227 |
3.227 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
35.702 |
| (<r2>)1/2 |
5.975 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at G4
| | hartrees |
| Energy at 0K | -131.346500 |
| Energy at 298.15K | -131.342008 |
| HF Energy | -131.404256 |
| Nuclear repulsion energy | 47.065841 |
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(2df,p)
| 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' |
3069 |
2961 |
8.20 |
|
|
|
| 2 |
A' |
2100 |
2027 |
21.16 |
|
|
|
| 3 |
A' |
1094 |
1056 |
39.34 |
|
|
|
| 4 |
A' |
942 |
909 |
42.13 |
|
|
|
| 5 |
A' |
467 |
451 |
23.10 |
|
|
|
| 6 |
A" |
335 |
323 |
12.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4003.5 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3863.4 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(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.048 |
-1.280 |
0.000 |
| C2 |
0.000 |
0.091 |
0.000 |
| N3 |
-0.197 |
1.254 |
0.000 |
| H4 |
1.088 |
-1.643 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3718 | 2.5458 | 1.1011 |
C2 | 1.3718 | | 1.1796 | 2.0473 | N3 | 2.5458 | 1.1796 | | 3.1694 | H4 | 1.1011 | 2.0473 | 3.1694 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.240 |
|
|
|
| 2 |
C |
0.317 |
|
|
|
| 3 |
N |
-0.268 |
|
|
|
| 4 |
H |
0.190 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.607 |
-1.401 |
0.000 |
2.132 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
36.056 |
| (<r2>)1/2 |
6.005 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at G4
| | hartrees |
| Energy at 0K | -131.346500 |
| Energy at 298.15K | -131.342008 |
| HF Energy | -131.404256 |
| Nuclear repulsion energy | 47.065841 |
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(2df,p)
Geometric Data calculated at B3LYP/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability