Jump to
S1C2
S2C1
S2C2
Energy calculated at PBEPBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.267533 |
| Energy at 298.15K | -131.266776 |
| HF Energy | -131.267533 |
| Nuclear repulsion energy | 47.076164 |
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 PBEPBE/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' |
3353 |
3318 |
44.25 |
|
|
|
| 2 |
A' |
1802 |
1783 |
28.65 |
|
|
|
| 3 |
A' |
1227 |
1215 |
3.93 |
|
|
|
| 4 |
A' |
450 |
445 |
8.75 |
|
|
|
| 5 |
A' |
341 |
337 |
42.74 |
|
|
|
| 6 |
A" |
447 |
442 |
1.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3809.5 cm
-1
Scaled (by 0.9897) Zero Point Vibrational Energy (zpe) 3770.3 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 PBEPBE/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.076 |
-1.221 |
0.000 |
| C2 |
0.000 |
0.082 |
0.000 |
| N3 |
-0.146 |
1.288 |
0.000 |
| H4 |
0.563 |
-2.180 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3058 | 2.5189 | 1.0754 |
C2 | 1.3058 | | 1.2143 | 2.3316 | N3 | 2.5189 | 1.2143 | | 3.5398 | H4 | 1.0754 | 2.3316 | 3.5398 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.455 |
|
C2 |
C1 |
H4 |
156.442 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at PBEPBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.267213 |
| Energy at 298.15K | |
| HF Energy | -131.267213 |
| Nuclear repulsion energy | 47.117725 |
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 PBEPBE/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 |
3406 |
3371 |
68.84 |
|
|
|
| 2 |
Σ |
1775 |
1756 |
28.91 |
|
|
|
| 3 |
Σ |
1250 |
1237 |
2.88 |
|
|
|
| 4 |
Π |
450 |
445 |
0.69 |
|
|
|
| 4 |
Π |
450 |
445 |
0.69 |
|
|
|
| 5 |
Π |
250i |
248i |
45.01 |
|
|
|
| 5 |
Π |
250i |
248i |
45.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3414.2 cm
-1
Scaled (by 0.9897) Zero Point Vibrational Energy (zpe) 3379.0 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 PBEPBE/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.215 |
| C2 |
0.000 |
0.000 |
0.080 |
| N3 |
0.000 |
0.000 |
1.299 |
| H4 |
0.000 |
0.000 |
-2.286 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2944 | 2.5142 | 1.0714 |
C2 | 1.2944 | | 1.2197 | 2.3658 | N3 | 2.5142 | 1.2197 | | 3.5855 | H4 | 1.0714 | 2.3658 | 3.5855 | |
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 PBEPBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.193 |
|
|
|
| 2 |
C |
0.319 |
|
|
|
| 3 |
N |
-0.359 |
|
|
|
| 4 |
H |
0.233 |
|
|
|
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 |
-3.170 |
3.170 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.858 |
0.000 |
0.000 |
| y |
0.000 |
-16.858 |
0.000 |
| z |
0.000 |
0.000 |
-15.052 |
|
| Traceless |
| | x | y | z |
| x |
-0.903 |
0.000 |
0.000 |
| y |
0.000 |
-0.903 |
0.000 |
| z |
0.000 |
0.000 |
1.806 |
|
| Polar |
| 3z2-r2 | 3.611 |
| 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 |
2.046 |
0.000 |
0.000 |
| y |
0.000 |
2.046 |
0.000 |
| z |
0.000 |
0.000 |
6.353 |
<r2> (average value of r
2) Å
2
| <r2> |
36.090 |
| (<r2>)1/2 |
6.008 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at PBEPBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.241137 |
| Energy at 298.15K | -131.240567 |
| HF Energy | -131.241137 |
| Nuclear repulsion energy | 46.693004 |
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 PBEPBE/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' |
3000 |
2969 |
9.20 |
|
|
|
| 2 |
A' |
2024 |
2003 |
16.47 |
|
|
|
| 3 |
A' |
1092 |
1081 |
20.74 |
|
|
|
| 4 |
A' |
897 |
887 |
59.51 |
|
|
|
| 5 |
A' |
454 |
450 |
21.13 |
|
|
|
| 6 |
A" |
310 |
307 |
10.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3888.5 cm
-1
Scaled (by 0.9897) Zero Point Vibrational Energy (zpe) 3848.4 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 PBEPBE/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.235 |
-1.262 |
0.000 |
| C2 |
0.000 |
0.088 |
0.000 |
| N3 |
-0.390 |
1.220 |
0.000 |
| H4 |
1.321 |
-1.494 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3709 | 2.5602 | 1.1101 |
C2 | 1.3709 | | 1.1975 | 2.0612 | N3 | 2.5602 | 1.1975 | | 3.2088 | H4 | 1.1101 | 2.0612 | 3.2088 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.258 |
|
|
|
| 2 |
C |
0.365 |
|
|
|
| 3 |
N |
-0.302 |
|
|
|
| 4 |
H |
0.195 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.728 |
-1.085 |
0.000 |
2.040 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.173 |
-1.606 |
0.000 |
| y |
-1.606 |
-20.793 |
0.000 |
| z |
0.000 |
0.000 |
-15.607 |
|
| Traceless |
| | x | y | z |
| x |
2.027 |
-1.606 |
0.000 |
| y |
-1.606 |
-4.903 |
0.000 |
| z |
0.000 |
0.000 |
2.876 |
|
| Polar |
| 3z2-r2 | 5.752 |
| x2-y2 | 4.620 |
| xy | -1.606 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.954 |
-1.184 |
0.000 |
| y |
-1.184 |
6.111 |
0.000 |
| z |
0.000 |
0.000 |
2.434 |
<r2> (average value of r
2) Å
2
| <r2> |
36.352 |
| (<r2>)1/2 |
6.029 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at PBEPBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.241137 |
| Energy at 298.15K | -131.240567 |
| HF Energy | -131.241137 |
| Nuclear repulsion energy | 46.693004 |
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 PBEPBE/6-31G(2df,p)
Geometric Data calculated at PBEPBE/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability