Jump to
S1C2
S2C1
S2C2
Energy calculated at B3PW91/6-31G**
| | hartrees |
| Energy at 0K | -131.367082 |
| Energy at 298.15K | -131.366408 |
| HF Energy | -131.367082 |
| Nuclear repulsion energy | 47.229018 |
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 B3PW91/6-31G**
| 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' |
3404 |
3263 |
36.06 |
|
|
|
| 2 |
A' |
1826 |
1750 |
33.07 |
|
|
|
| 3 |
A' |
1239 |
1188 |
7.50 |
|
|
|
| 4 |
A' |
487 |
467 |
28.70 |
|
|
|
| 5 |
A' |
392 |
376 |
19.25 |
|
|
|
| 6 |
A" |
448 |
430 |
1.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3898.3 cm
-1
Scaled (by 0.9584) Zero Point Vibrational Energy (zpe) 3736.1 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 B3PW91/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.074 |
-1.224 |
0.000 |
| C2 |
0.000 |
0.086 |
0.000 |
| N3 |
-0.155 |
1.279 |
0.000 |
| H4 |
0.640 |
-2.134 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3121 | 2.5135 | 1.0718 |
C2 | 1.3121 | | 1.2030 | 2.3107 | N3 | 2.5135 | 1.2030 | | 3.5047 | H4 | 1.0718 | 2.3107 | 3.5047 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.835 |
|
C2 |
C1 |
H4 |
151.370 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3PW91/6-31G**
| | hartrees |
| Energy at 0K | -131.366403 |
| Energy at 298.15K | |
| HF Energy | -131.366403 |
| Nuclear repulsion energy | 47.287016 |
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 B3PW91/6-31G**
| 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 |
3465 |
3321 |
69.34 |
|
|
|
| 2 |
Σ |
1761 |
1688 |
36.31 |
|
|
|
| 3 |
Σ |
1281 |
1228 |
5.27 |
|
|
|
| 4 |
Π |
451 |
432 |
0.94 |
|
|
|
| 4 |
Π |
451 |
432 |
0.94 |
|
|
|
| 5 |
Π |
297i |
284i |
50.99 |
|
|
|
| 5 |
Π |
297i |
284i |
50.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3407.9 cm
-1
Scaled (by 0.9584) Zero Point Vibrational Energy (zpe) 3266.1 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 B3PW91/6-31G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.212 |
| C2 |
0.000 |
0.000 |
0.082 |
| N3 |
0.000 |
0.000 |
1.294 |
| H4 |
0.000 |
0.000 |
-2.279 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2941 | 2.5060 | 1.0670 |
C2 | 1.2941 | | 1.2119 | 2.3610 | N3 | 2.5060 | 1.2119 | | 3.5729 | H4 | 1.0670 | 2.3610 | 3.5729 | |
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 B3PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.039 |
|
|
|
| 2 |
C |
0.287 |
|
|
|
| 3 |
N |
-0.482 |
|
|
|
| 4 |
H |
0.234 |
|
|
|
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 |
-3.288 |
3.288 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.867 |
0.000 |
0.000 |
| y |
0.000 |
-16.867 |
0.000 |
| z |
0.000 |
0.000 |
-15.101 |
|
| Traceless |
| | x | y | z |
| x |
-0.883 |
0.000 |
0.000 |
| y |
0.000 |
-0.883 |
0.000 |
| z |
0.000 |
0.000 |
1.766 |
|
| Polar |
| 3z2-r2 | 3.533 |
| 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 |
1.640 |
0.000 |
0.000 |
| y |
0.000 |
1.640 |
0.000 |
| z |
0.000 |
0.000 |
6.173 |
<r2> (average value of r
2) Å
2
| <r2> |
35.935 |
| (<r2>)1/2 |
5.995 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3PW91/6-31G**
| | hartrees |
| Energy at 0K | -131.335918 |
| Energy at 298.15K | -131.335354 |
| HF Energy | -131.335918 |
| Nuclear repulsion energy | 46.924109 |
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 B3PW91/6-31G**
| 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' |
3085 |
2956 |
11.42 |
|
|
|
| 2 |
A' |
2113 |
2025 |
17.75 |
|
|
|
| 3 |
A' |
1103 |
1057 |
32.11 |
|
|
|
| 4 |
A' |
925 |
887 |
54.45 |
|
|
|
| 5 |
A' |
444 |
425 |
23.31 |
|
|
|
| 6 |
A" |
319 |
306 |
9.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3994.4 cm
-1
Scaled (by 0.9584) Zero Point Vibrational Energy (zpe) 3828.3 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 B3PW91/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.130 |
-1.277 |
0.000 |
| C2 |
0.000 |
0.091 |
0.000 |
| N3 |
-0.281 |
1.242 |
0.000 |
| H4 |
1.189 |
-1.578 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3743 | 2.5524 | 1.1014 |
C2 | 1.3743 | | 1.1849 | 2.0495 | N3 | 2.5524 | 1.1849 | | 3.1805 | H4 | 1.1014 | 2.0495 | 3.1805 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.087 |
|
|
|
| 2 |
C |
0.325 |
|
|
|
| 3 |
N |
-0.414 |
|
|
|
| 4 |
H |
0.177 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.814 |
-1.338 |
0.000 |
2.255 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.440 |
-2.180 |
0.000 |
| y |
-2.180 |
-20.763 |
0.000 |
| z |
0.000 |
0.000 |
-15.531 |
|
| Traceless |
| | x | y | z |
| x |
1.707 |
-2.180 |
0.000 |
| y |
-2.180 |
-4.777 |
0.000 |
| z |
0.000 |
0.000 |
3.071 |
|
| Polar |
| 3z2-r2 | 6.141 |
| x2-y2 | 4.323 |
| xy | -2.180 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.479 |
-0.940 |
0.000 |
| y |
-0.940 |
6.060 |
0.000 |
| z |
0.000 |
0.000 |
2.189 |
<r2> (average value of r
2) Å
2
| <r2> |
36.173 |
| (<r2>)1/2 |
6.014 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3PW91/6-31G**
| | hartrees |
| Energy at 0K | -131.335918 |
| Energy at 298.15K | -131.335354 |
| HF Energy | -131.335918 |
| Nuclear repulsion energy | 46.924109 |
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 B3PW91/6-31G**
Geometric Data calculated at B3PW91/6-31G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability