Jump to
S1C2
S2C1
S2C2
Energy calculated at PBE1PBE/6-31G*
| | hartrees |
| Energy at 0K | -131.262906 |
| Energy at 298.15K | -131.262240 |
| HF Energy | -131.262906 |
| Nuclear repulsion energy | 47.264109 |
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 PBE1PBE/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' |
3424 |
3253 |
33.28 |
|
|
|
| 2 |
A' |
1834 |
1743 |
36.04 |
|
|
|
| 3 |
A' |
1243 |
1182 |
8.01 |
|
|
|
| 4 |
A' |
498 |
473 |
31.84 |
|
|
|
| 5 |
A' |
396 |
376 |
16.50 |
|
|
|
| 6 |
A" |
450 |
427 |
1.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3922.2 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 3727.3 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 PBE1PBE/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.071 |
-1.224 |
0.000 |
| C2 |
0.000 |
0.087 |
0.000 |
| N3 |
-0.154 |
1.278 |
0.000 |
| H4 |
0.649 |
-2.127 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3125 | 2.5118 | 1.0723 |
C2 | 1.3125 | | 1.2010 | 2.3070 | N3 | 2.5118 | 1.2010 | | 3.4983 | H4 | 1.0723 | 2.3070 | 3.4983 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.752 |
|
C2 |
C1 |
H4 |
150.492 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at PBE1PBE/6-31G*
| | hartrees |
| Energy at 0K | -131.262126 |
| Energy at 298.15K | |
| HF Energy | -131.262126 |
| Nuclear repulsion energy | 47.325608 |
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 PBE1PBE/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 |
3483 |
3310 |
65.54 |
|
|
|
| 2 |
Σ |
1762 |
1674 |
40.49 |
|
|
|
| 3 |
Σ |
1289 |
1225 |
5.53 |
|
|
|
| 4 |
Π |
451 |
429 |
0.82 |
|
|
|
| 4 |
Π |
451 |
429 |
0.82 |
|
|
|
| 5 |
Π |
307i |
292i |
52.24 |
|
|
|
| 5 |
Π |
307i |
292i |
52.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3411.5 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 3241.9 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 PBE1PBE/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 |
0.082 |
| N3 |
0.000 |
0.000 |
1.293 |
| H4 |
0.000 |
0.000 |
-2.278 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2931 | 2.5037 | 1.0676 |
C2 | 1.2931 | | 1.2106 | 2.3606 | N3 | 2.5037 | 1.2106 | | 3.5712 | H4 | 1.0676 | 2.3606 | 3.5712 | |
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 PBE1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.091 |
|
|
|
| 2 |
C |
0.282 |
|
|
|
| 3 |
N |
-0.467 |
|
|
|
| 4 |
H |
0.276 |
|
|
|
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 |
-3.304 |
3.304 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.926 |
0.000 |
0.000 |
| y |
0.000 |
-16.926 |
0.000 |
| z |
0.000 |
0.000 |
-15.056 |
|
| Traceless |
| | x | y | z |
| x |
-0.935 |
0.000 |
0.000 |
| y |
0.000 |
-0.935 |
0.000 |
| z |
0.000 |
0.000 |
1.870 |
|
| Polar |
| 3z2-r2 | 3.741 |
| 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 |
1.629 |
0.000 |
0.000 |
| y |
0.000 |
1.629 |
0.000 |
| z |
0.000 |
0.000 |
6.114 |
<r2> (average value of r
2) Å
2
| <r2> |
35.910 |
| (<r2>)1/2 |
5.993 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at PBE1PBE/6-31G*
| | hartrees |
| Energy at 0K | -131.229635 |
| Energy at 298.15K | -131.229072 |
| HF Energy | -131.229635 |
| Nuclear repulsion energy | 46.965791 |
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 PBE1PBE/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' |
3109 |
2955 |
11.78 |
|
|
|
| 2 |
A' |
2135 |
2029 |
18.94 |
|
|
|
| 3 |
A' |
1109 |
1054 |
36.18 |
|
|
|
| 4 |
A' |
938 |
892 |
52.91 |
|
|
|
| 5 |
A' |
446 |
424 |
23.41 |
|
|
|
| 6 |
A" |
320 |
304 |
10.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4028.8 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 3828.6 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 PBE1PBE/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.116 |
-1.278 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.266 |
1.244 |
0.000 |
| H4 |
1.170 |
-1.592 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3748 | 2.5507 | 1.1006 |
C2 | 1.3748 | | 1.1824 | 2.0510 | N3 | 2.5507 | 1.1824 | | 3.1793 | H4 | 1.1006 | 2.0510 | 3.1793 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.127 |
|
|
|
| 2 |
C |
0.315 |
|
|
|
| 3 |
N |
-0.404 |
|
|
|
| 4 |
H |
0.216 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.829 |
-1.354 |
0.000 |
2.276 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.520 |
-2.277 |
0.000 |
| y |
-2.277 |
-20.793 |
0.000 |
| z |
0.000 |
0.000 |
-15.574 |
|
| Traceless |
| | x | y | z |
| x |
1.663 |
-2.277 |
0.000 |
| y |
-2.277 |
-4.746 |
0.000 |
| z |
0.000 |
0.000 |
3.082 |
|
| Polar |
| 3z2-r2 | 6.165 |
| x2-y2 | 4.273 |
| xy | -2.277 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.431 |
-0.894 |
0.000 |
| y |
-0.894 |
6.044 |
0.000 |
| z |
0.000 |
0.000 |
2.186 |
<r2> (average value of r
2) Å
2
| <r2> |
36.174 |
| (<r2>)1/2 |
6.015 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at PBE1PBE/6-31G*
| | hartrees |
| Energy at 0K | -131.229635 |
| Energy at 298.15K | -131.229072 |
| HF Energy | -131.229635 |
| Nuclear repulsion energy | 46.965791 |
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 PBE1PBE/6-31G*
Geometric Data calculated at PBE1PBE/6-31G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability