Jump to
S1C2
S2C1
S2C2
Energy calculated at B2PLYP/6-31+G**
| | hartrees |
| Energy at 0K | -131.296266 |
| Energy at 298.15K | -131.295662 |
| HF Energy | -131.175792 |
| Nuclear repulsion energy | 47.177596 |
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 B2PLYP/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' |
3395 |
3234 |
29.90 |
|
|
|
| 2 |
A' |
1891 |
1801 |
17.97 |
|
|
|
| 3 |
A' |
1186 |
1130 |
13.95 |
|
|
|
| 4 |
A' |
588 |
560 |
33.45 |
|
|
|
| 5 |
A' |
399 |
380 |
8.07 |
|
|
|
| 6 |
A" |
441 |
420 |
1.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3950.5 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 3762.5 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 B2PLYP/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.021 |
-1.236 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.110 |
1.282 |
0.000 |
| H4 |
0.638 |
-2.112 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3283 | 2.5209 | 1.0717 |
C2 | 1.3283 | | 1.1944 | 2.2950 | N3 | 2.5209 | 1.1944 | | 3.4752 | H4 | 1.0717 | 2.2950 | 3.4752 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.661 |
|
C2 |
C1 |
H4 |
145.767 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B2PLYP/6-31+G**
| | hartrees |
| Energy at 0K | -131.294699 |
| Energy at 298.15K | |
| HF Energy | -131.175039 |
| Nuclear repulsion energy | 47.296190 |
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 B2PLYP/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 |
3475 |
3309 |
74.98 |
|
|
|
| 2 |
Σ |
1721 |
1639 |
28.32 |
|
|
|
| 3 |
Σ |
1271 |
1211 |
9.63 |
|
|
|
| 4 |
Π |
443 |
422 |
0.09 |
|
|
|
| 4 |
Π |
443 |
422 |
0.09 |
|
|
|
| 5 |
Π |
398i |
379i |
64.19 |
|
|
|
| 5 |
Π |
398i |
379i |
64.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3278.9 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 3122.8 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 B2PLYP/6-31+G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.213 |
| C2 |
0.000 |
0.000 |
0.084 |
| N3 |
0.000 |
0.000 |
1.293 |
| H4 |
0.000 |
0.000 |
-2.279 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2976 | 2.5064 | 1.0652 |
C2 | 1.2976 | | 1.2088 | 2.3629 | N3 | 2.5064 | 1.2088 | | 3.5717 | H4 | 1.0652 | 2.3629 | 3.5717 | |
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 B2PLYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.239 |
|
|
|
| 2 |
C |
-0.040 |
|
|
|
| 3 |
N |
-0.451 |
|
|
|
| 4 |
H |
0.252 |
|
|
|
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 |
-3.460 |
3.460 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.621 |
0.000 |
0.000 |
| y |
0.000 |
-17.621 |
0.000 |
| z |
0.000 |
0.000 |
-16.015 |
|
| Traceless |
| | x | y | z |
| x |
-0.803 |
0.000 |
0.000 |
| y |
0.000 |
-0.803 |
0.000 |
| z |
0.000 |
0.000 |
1.605 |
|
| Polar |
| 3z2-r2 | 3.211 |
| 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 |
2.217 |
0.000 |
0.000 |
| y |
0.000 |
2.217 |
0.000 |
| z |
0.000 |
0.000 |
7.023 |
<r2> (average value of r
2) Å
2
| <r2> |
36.444 |
| (<r2>)1/2 |
6.037 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B2PLYP/6-31+G**
| | hartrees |
| Energy at 0K | -131.275679 |
| Energy at 298.15K | -131.275086 |
| HF Energy | -131.139339 |
| Nuclear repulsion energy | 46.716205 |
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 B2PLYP/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' |
3112 |
2964 |
8.18 |
|
|
|
| 2 |
A' |
2086 |
1987 |
21.38 |
|
|
|
| 3 |
A' |
1077 |
1026 |
42.67 |
|
|
|
| 4 |
A' |
952 |
907 |
40.04 |
|
|
|
| 5 |
A' |
417 |
397 |
23.12 |
|
|
|
| 6 |
A" |
312 |
297 |
7.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3978.3 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 3788.9 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 B2PLYP/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.209 |
-1.274 |
0.000 |
| C2 |
0.000 |
0.093 |
0.000 |
| N3 |
-0.362 |
1.227 |
0.000 |
| H4 |
1.283 |
-1.500 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3836 | 2.5656 | 1.0977 |
C2 | 1.3836 | | 1.1900 | 2.0456 | N3 | 2.5656 | 1.1900 | | 3.1847 | H4 | 1.0977 | 2.0456 | 3.1847 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.171 |
|
|
|
| 2 |
C |
0.335 |
|
|
|
| 3 |
N |
-0.324 |
|
|
|
| 4 |
H |
0.160 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.029 |
-1.219 |
0.000 |
2.367 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.911 |
-2.150 |
0.000 |
| y |
-2.150 |
-22.311 |
0.000 |
| z |
0.000 |
0.000 |
-16.198 |
|
| Traceless |
| | x | y | z |
| x |
2.344 |
-2.150 |
0.000 |
| y |
-2.150 |
-5.757 |
0.000 |
| z |
0.000 |
0.000 |
3.413 |
|
| Polar |
| 3z2-r2 | 6.826 |
| x2-y2 | 5.401 |
| xy | -2.150 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.118 |
-0.991 |
0.000 |
| y |
-0.991 |
6.890 |
0.000 |
| z |
0.000 |
0.000 |
2.763 |
<r2> (average value of r
2) Å
2
| <r2> |
36.947 |
| (<r2>)1/2 |
6.078 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B2PLYP/6-31+G**
| | hartrees |
| Energy at 0K | -131.275679 |
| Energy at 298.15K | -131.275086 |
| HF Energy | -131.139339 |
| Nuclear repulsion energy | 46.716205 |
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 B2PLYP/6-31+G**
Geometric Data calculated at B2PLYP/6-31+G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability