Jump to
S1C2
S2C1
S2C2
Energy calculated at mPW1PW91/6-31G**
| | hartrees |
| Energy at 0K | -131.385369 |
| Energy at 298.15K | -131.384705 |
| HF Energy | -131.385369 |
| Nuclear repulsion energy | 47.290508 |
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 mPW1PW91/6-31G**
| 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' |
3421 |
3255 |
36.12 |
|
|
|
| 2 |
A' |
1829 |
1741 |
36.43 |
|
|
|
| 3 |
A' |
1242 |
1182 |
8.25 |
|
|
|
| 4 |
A' |
495 |
471 |
29.37 |
|
|
|
| 5 |
A' |
395 |
376 |
16.57 |
|
|
|
| 6 |
A" |
449 |
428 |
1.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3915.4 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 3725.5 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 mPW1PW91/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.075 |
-1.223 |
0.000 |
| C2 |
0.000 |
0.087 |
0.000 |
| N3 |
-0.157 |
1.277 |
0.000 |
| H4 |
0.649 |
-2.126 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3120 | 2.5106 | 1.0704 |
C2 | 1.3120 | | 1.2003 | 2.3065 | N3 | 2.5106 | 1.2003 | | 3.4974 | H4 | 1.0704 | 2.3065 | 3.4974 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.760 |
|
C2 |
C1 |
H4 |
150.836 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at mPW1PW91/6-31G**
| | hartrees |
| Energy at 0K | -131.384636 |
| Energy at 298.15K | |
| HF Energy | -131.384636 |
| Nuclear repulsion energy | 47.350972 |
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 mPW1PW91/6-31G**
| 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 |
3482 |
3313 |
70.22 |
|
|
|
| 2 |
Σ |
1757 |
1672 |
40.63 |
|
|
|
| 3 |
Σ |
1287 |
1225 |
5.68 |
|
|
|
| 4 |
Π |
452 |
430 |
0.86 |
|
|
|
| 4 |
Π |
452 |
430 |
0.86 |
|
|
|
| 5 |
Π |
303i |
288i |
50.75 |
|
|
|
| 5 |
Π |
303i |
288i |
50.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3412.0 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 3246.5 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 mPW1PW91/6-31G**
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 |
1.292 |
| H4 |
0.000 |
0.000 |
-2.276 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2929 | 2.5027 | 1.0655 |
C2 | 1.2929 | | 1.2098 | 2.3584 | N3 | 2.5027 | 1.2098 | | 3.5682 | H4 | 1.0655 | 2.3584 | 3.5682 | |
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 mPW1PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.038 |
|
|
|
| 2 |
C |
0.281 |
|
|
|
| 3 |
N |
-0.481 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
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 |
-3.294 |
3.294 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.875 |
0.000 |
0.000 |
| y |
0.000 |
-16.875 |
0.000 |
| z |
0.000 |
0.000 |
-15.086 |
|
| Traceless |
| | x | y | z |
| x |
-0.895 |
0.000 |
0.000 |
| y |
0.000 |
-0.895 |
0.000 |
| z |
0.000 |
0.000 |
1.790 |
|
| Polar |
| 3z2-r2 | 3.579 |
| 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 |
1.638 |
0.000 |
0.000 |
| y |
0.000 |
1.638 |
0.000 |
| z |
0.000 |
0.000 |
6.129 |
<r2> (average value of r
2) Å
2
| <r2> |
35.868 |
| (<r2>)1/2 |
5.989 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at mPW1PW91/6-31G**
| | hartrees |
| Energy at 0K | -131.352029 |
| Energy at 298.15K | -131.351471 |
| HF Energy | -131.352029 |
| Nuclear repulsion energy | 46.999560 |
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 mPW1PW91/6-31G**
| 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' |
3106 |
2955 |
10.56 |
|
|
|
| 2 |
A' |
2135 |
2032 |
18.98 |
|
|
|
| 3 |
A' |
1105 |
1051 |
35.13 |
|
|
|
| 4 |
A' |
934 |
888 |
51.54 |
|
|
|
| 5 |
A' |
445 |
424 |
24.01 |
|
|
|
| 6 |
A" |
321 |
306 |
10.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4023.0 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 3827.8 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 mPW1PW91/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.096 |
-1.280 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.246 |
1.247 |
0.000 |
| H4 |
1.148 |
-1.601 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3745 | 2.5496 | 1.0996 |
C2 | 1.3745 | | 1.1813 | 2.0453 | N3 | 2.5496 | 1.1813 | | 3.1711 | H4 | 1.0996 | 2.0453 | 3.1711 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.082 |
|
|
|
| 2 |
C |
0.319 |
|
|
|
| 3 |
N |
-0.416 |
|
|
|
| 4 |
H |
0.179 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.794 |
-1.394 |
0.000 |
2.272 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.546 |
-2.310 |
0.000 |
| y |
-2.310 |
-20.687 |
0.000 |
| z |
0.000 |
0.000 |
-15.538 |
|
| Traceless |
| | x | y | z |
| x |
1.566 |
-2.310 |
0.000 |
| y |
-2.310 |
-4.644 |
0.000 |
| z |
0.000 |
0.000 |
3.078 |
|
| Polar |
| 3z2-r2 | 6.157 |
| x2-y2 | 4.140 |
| xy | -2.310 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.419 |
-0.835 |
0.000 |
| y |
-0.835 |
6.061 |
0.000 |
| z |
0.000 |
0.000 |
2.194 |
<r2> (average value of r
2) Å
2
| <r2> |
36.106 |
| (<r2>)1/2 |
6.009 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at mPW1PW91/6-31G**
| | hartrees |
| Energy at 0K | -131.352029 |
| Energy at 298.15K | -131.351471 |
| HF Energy | -131.352029 |
| Nuclear repulsion energy | 46.999560 |
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 mPW1PW91/6-31G**
Geometric Data calculated at mPW1PW91/6-31G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability