Jump to
S1C2
S2C1
S2C2
Energy calculated at B3PW91/6-31+G**
| | hartrees |
| Energy at 0K | -131.372379 |
| Energy at 298.15K | -131.371681 |
| HF Energy | -131.372379 |
| Nuclear repulsion energy | 47.216219 |
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 B3PW91/6-31+G**
| 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' |
3403 |
3267 |
39.81 |
|
|
|
| 2 |
A' |
1818 |
1745 |
32.86 |
|
|
|
| 3 |
A' |
1237 |
1188 |
7.55 |
|
|
|
| 4 |
A' |
473 |
455 |
24.89 |
|
|
|
| 5 |
A' |
384 |
368 |
24.30 |
|
|
|
| 6 |
A" |
440 |
423 |
0.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3877.4 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 3722.7 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 B3PW91/6-31+G**
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 |
-0.150 |
1.281 |
0.000 |
| H4 |
0.622 |
-2.143 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3121 | 2.5140 | 1.0721 |
C2 | 1.3121 | | 1.2034 | 2.3149 | N3 | 2.5140 | 1.2034 | | 3.5097 | H4 | 1.0721 | 2.3149 | 3.5097 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.952 |
|
C2 |
C1 |
H4 |
152.145 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3PW91/6-31+G**
| | hartrees |
| Energy at 0K | -131.371797 |
| Energy at 298.15K | |
| HF Energy | -131.371797 |
| Nuclear repulsion energy | 47.269737 |
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 B3PW91/6-31+G**
| 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 |
3456 |
3318 |
71.15 |
|
|
|
| 2 |
Σ |
1756 |
1686 |
35.07 |
|
|
|
| 3 |
Σ |
1277 |
1226 |
5.00 |
|
|
|
| 4 |
Π |
446 |
428 |
0.36 |
|
|
|
| 4 |
Π |
446 |
428 |
0.36 |
|
|
|
| 5 |
Π |
277i |
265i |
61.03 |
|
|
|
| 5 |
Π |
277i |
265i |
61.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3414.0 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 3277.8 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 B3PW91/6-31+G**
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 |
-2.280 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2949 | 2.5068 | 1.0679 |
C2 | 1.2949 | | 1.2119 | 2.3628 | N3 | 2.5068 | 1.2119 | | 3.5747 | H4 | 1.0679 | 2.3628 | 3.5747 | |
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 B3PW91/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.334 |
|
|
|
| 2 |
C |
-0.138 |
|
|
|
| 3 |
N |
-0.456 |
|
|
|
| 4 |
H |
0.260 |
|
|
|
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 |
-3.371 |
3.371 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.415 |
0.000 |
0.000 |
| y |
0.000 |
-17.415 |
0.000 |
| z |
0.000 |
0.000 |
-15.632 |
|
| Traceless |
| | x | y | z |
| x |
-0.891 |
0.000 |
0.000 |
| y |
0.000 |
-0.891 |
0.000 |
| z |
0.000 |
0.000 |
1.782 |
|
| Polar |
| 3z2-r2 | 3.565 |
| 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 |
2.180 |
0.000 |
0.000 |
| y |
0.000 |
2.180 |
0.000 |
| z |
0.000 |
0.000 |
6.998 |
<r2> (average value of r
2) Å
2
| <r2> |
36.295 |
| (<r2>)1/2 |
6.025 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3PW91/6-31+G**
| | hartrees |
| Energy at 0K | -131.341982 |
| Energy at 298.15K | -131.341402 |
| HF Energy | -131.341982 |
| Nuclear repulsion energy | 46.915525 |
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 B3PW91/6-31+G**
| 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' |
3089 |
2966 |
6.17 |
|
|
|
| 2 |
A' |
2107 |
2023 |
17.44 |
|
|
|
| 3 |
A' |
1097 |
1053 |
32.70 |
|
|
|
| 4 |
A' |
921 |
884 |
54.99 |
|
|
|
| 5 |
A' |
436 |
419 |
26.36 |
|
|
|
| 6 |
A" |
312 |
299 |
7.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3980.4 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 3821.5 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 B3PW91/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.160 |
-1.274 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.313 |
1.235 |
0.000 |
| H4 |
1.226 |
-1.549 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3753 | 2.5529 | 1.1009 |
C2 | 1.3753 | | 1.1848 | 2.0483 | N3 | 2.5529 | 1.1848 | | 3.1806 | H4 | 1.1009 | 2.0483 | 3.1806 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.130 |
|
|
|
| 2 |
C |
0.286 |
|
|
|
| 3 |
N |
-0.335 |
|
|
|
| 4 |
H |
0.178 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.975 |
-1.302 |
0.000 |
2.366 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.810 |
-2.365 |
0.000 |
| y |
-2.365 |
-21.675 |
0.000 |
| z |
0.000 |
0.000 |
-16.030 |
|
| Traceless |
| | x | y | z |
| x |
2.042 |
-2.365 |
0.000 |
| y |
-2.365 |
-5.255 |
0.000 |
| z |
0.000 |
0.000 |
3.213 |
|
| Polar |
| 3z2-r2 | 6.425 |
| x2-y2 | 4.865 |
| xy | -2.365 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.999 |
-0.866 |
0.000 |
| y |
-0.866 |
6.975 |
0.000 |
| z |
0.000 |
0.000 |
2.720 |
<r2> (average value of r
2) Å
2
| <r2> |
36.552 |
| (<r2>)1/2 |
6.046 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3PW91/6-31+G**
| | hartrees |
| Energy at 0K | -131.341982 |
| Energy at 298.15K | -131.341402 |
| HF Energy | -131.341982 |
| Nuclear repulsion energy | 46.915525 |
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 B3PW91/6-31+G**
Geometric Data calculated at B3PW91/6-31+G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability