Jump to
S1C2
S2C1
S2C2
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.372183 |
| Energy at 298.15K | -131.371388 |
| HF Energy | -131.372183 |
| Nuclear repulsion energy | 47.557114 |
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 B1B95/6-31G(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' |
3443 |
3297 |
50.09 |
|
|
|
| 2 |
A' |
1779 |
1704 |
40.55 |
|
|
|
| 3 |
A' |
1265 |
1212 |
7.24 |
|
|
|
| 4 |
A' |
459 |
440 |
4.30 |
|
|
|
| 5 |
A' |
289 |
277 |
46.17 |
|
|
|
| 6 |
A" |
460 |
441 |
1.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3847.6 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 3684.9 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 B1B95/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.098 |
-1.207 |
0.000 |
| C2 |
0.000 |
0.083 |
0.000 |
| N3 |
-0.164 |
1.273 |
0.000 |
| H4 |
0.559 |
-2.167 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2938 | 2.4930 | 1.0658 |
C2 | 1.2938 | | 1.2004 | 2.3192 | N3 | 2.4930 | 1.2004 | | 3.5151 | H4 | 1.0658 | 2.3192 | 3.5151 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.495 |
|
C2 |
C1 |
H4 |
158.664 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.372018 |
| Energy at 298.15K | |
| HF Energy | -131.372018 |
| Nuclear repulsion energy | 47.595015 |
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 B1B95/6-31G(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 |
3485 |
3337 |
70.04 |
|
|
|
| 2 |
Σ |
1739 |
1666 |
43.39 |
|
|
|
| 3 |
Σ |
1290 |
1236 |
5.12 |
|
|
|
| 4 |
Π |
461 |
442 |
0.69 |
|
|
|
| 4 |
Π |
461 |
442 |
0.69 |
|
|
|
| 5 |
Π |
195i |
186i |
47.32 |
|
|
|
| 5 |
Π |
195i |
186i |
47.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3524.0 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 3374.9 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 B1B95/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.203 |
| C2 |
0.000 |
0.000 |
0.080 |
| N3 |
0.000 |
0.000 |
1.286 |
| H4 |
0.000 |
0.000 |
-2.265 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2825 | 2.4887 | 1.0627 |
C2 | 1.2825 | | 1.2063 | 2.3452 | N3 | 2.4887 | 1.2063 | | 3.5514 | H4 | 1.0627 | 2.3452 | 3.5514 | |
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 B1B95/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.223 |
|
|
|
| 2 |
C |
0.308 |
|
|
|
| 3 |
N |
-0.335 |
|
|
|
| 4 |
H |
0.250 |
|
|
|
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 |
-3.239 |
3.239 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.804 |
0.000 |
0.000 |
| y |
0.000 |
-16.804 |
0.000 |
| z |
0.000 |
0.000 |
-14.966 |
|
| Traceless |
| | x | y | z |
| x |
-0.919 |
0.000 |
0.000 |
| y |
0.000 |
-0.919 |
0.000 |
| z |
0.000 |
0.000 |
1.838 |
|
| Polar |
| 3z2-r2 | 3.675 |
| 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 |
2.017 |
0.000 |
0.000 |
| y |
0.000 |
2.017 |
0.000 |
| z |
0.000 |
0.000 |
6.216 |
<r2> (average value of r
2) Å
2
| <r2> |
35.539 |
| (<r2>)1/2 |
5.961 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.345859 |
| Energy at 298.15K | -131.345328 |
| HF Energy | -131.345859 |
| Nuclear repulsion energy | 47.169052 |
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 B1B95/6-31G(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' |
3084 |
2953 |
7.66 |
|
|
|
| 2 |
A' |
2129 |
2039 |
23.16 |
|
|
|
| 3 |
A' |
1097 |
1051 |
39.33 |
|
|
|
| 4 |
A' |
945 |
905 |
40.46 |
|
|
|
| 5 |
A' |
464 |
445 |
23.90 |
|
|
|
| 6 |
A" |
326 |
312 |
13.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4022.7 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 3852.5 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 B1B95/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.034 |
-1.279 |
0.000 |
| C2 |
0.000 |
0.091 |
0.000 |
| N3 |
-0.182 |
1.253 |
0.000 |
| H4 |
1.073 |
-1.639 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3708 | 2.5410 | 1.1002 |
C2 | 1.3708 | | 1.1756 | 2.0361 | N3 | 2.5410 | 1.1756 | | 3.1525 | H4 | 1.1002 | 2.0361 | 3.1525 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.240 |
|
|
|
| 2 |
C |
0.321 |
|
|
|
| 3 |
N |
-0.278 |
|
|
|
| 4 |
H |
0.197 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.597 |
-1.402 |
0.000 |
2.126 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.650 |
-2.312 |
0.000 |
| y |
-2.312 |
-20.369 |
0.000 |
| z |
0.000 |
0.000 |
-15.564 |
|
| Traceless |
| | x | y | z |
| x |
1.316 |
-2.312 |
0.000 |
| y |
-2.312 |
-4.262 |
0.000 |
| z |
0.000 |
0.000 |
2.946 |
|
| Polar |
| 3z2-r2 | 5.892 |
| x2-y2 | 3.718 |
| xy | -2.312 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.603 |
-0.610 |
0.000 |
| y |
-0.610 |
6.139 |
0.000 |
| z |
0.000 |
0.000 |
2.444 |
<r2> (average value of r
2) Å
2
| <r2> |
35.877 |
| (<r2>)1/2 |
5.990 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.345859 |
| Energy at 298.15K | -131.345328 |
| HF Energy | -131.345859 |
| Nuclear repulsion energy | 47.169052 |
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 B1B95/6-31G(2df,p)
Geometric Data calculated at B1B95/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability