Jump to
S1C2
S2C1
S2C2
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -131.322081 |
| Energy at 298.15K | -131.321501 |
| HF Energy | -131.198768 |
| Nuclear repulsion energy | 47.396118 |
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/6-311G*
| 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' |
3368 |
3368 |
22.97 |
|
|
|
| 2 |
A' |
1890 |
1890 |
20.44 |
|
|
|
| 3 |
A' |
1174 |
1174 |
14.18 |
|
|
|
| 4 |
A' |
583 |
583 |
34.19 |
|
|
|
| 5 |
A' |
409 |
409 |
10.09 |
|
|
|
| 6 |
A" |
465 |
465 |
2.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3944.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3944.2 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.016 |
-1.231 |
0.000 |
| C2 |
0.000 |
0.094 |
0.000 |
| N3 |
-0.068 |
1.278 |
0.000 |
| H4 |
0.575 |
-2.124 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3245 | 2.5092 | 1.0712 |
C2 | 1.3245 | | 1.1863 | 2.2909 | N3 | 2.5092 | 1.1863 | | 3.4621 | H4 | 1.0712 | 2.2909 | 3.4621 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.000 |
|
C2 |
C1 |
H4 |
145.788 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -131.320699 |
| Energy at 298.15K | |
| HF Energy | -131.197991 |
| Nuclear repulsion energy | 47.528705 |
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/6-311G*
| 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 |
3458 |
3458 |
62.24 |
|
|
|
| 2 |
Σ |
1716 |
1716 |
30.21 |
|
|
|
| 3 |
Σ |
1258 |
1258 |
10.81 |
|
|
|
| 4 |
Π |
466 |
466 |
0.47 |
|
|
|
| 4 |
Π |
466 |
466 |
0.47 |
|
|
|
| 5 |
Π |
356i |
356i |
55.05 |
|
|
|
| 5 |
Π |
356i |
356i |
55.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3325.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3325.1 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 B2PLYP/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.208 |
| C2 |
0.000 |
0.000 |
0.086 |
| N3 |
0.000 |
0.000 |
1.286 |
| H4 |
0.000 |
0.000 |
-2.272 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2934 | 2.4938 | 1.0639 |
C2 | 1.2934 | | 1.2004 | 2.3573 | N3 | 2.4938 | 1.2004 | | 3.5577 | H4 | 1.0639 | 2.3573 | 3.5577 | |
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/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.081 |
|
|
|
| 2 |
C |
0.009 |
|
|
|
| 3 |
N |
-0.224 |
|
|
|
| 4 |
H |
0.295 |
|
|
|
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 |
-3.351 |
3.351 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.334 |
0.000 |
0.000 |
| y |
0.000 |
-17.334 |
0.000 |
| z |
0.000 |
0.000 |
-15.498 |
|
| Traceless |
| | x | y | z |
| x |
-0.918 |
0.000 |
0.000 |
| y |
0.000 |
-0.918 |
0.000 |
| z |
0.000 |
0.000 |
1.836 |
|
| Polar |
| 3z2-r2 | 3.672 |
| 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 |
1.886 |
0.000 |
0.000 |
| y |
0.000 |
1.886 |
0.000 |
| z |
0.000 |
0.000 |
6.258 |
<r2> (average value of r
2) Å
2
| <r2> |
35.978 |
| (<r2>)1/2 |
5.998 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -131.301786 |
| Energy at 298.15K | -131.301244 |
| HF Energy | -131.163325 |
| Nuclear repulsion energy | 46.912737 |
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/6-311G*
| 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' |
3097 |
3097 |
12.18 |
|
|
|
| 2 |
A' |
2084 |
2084 |
25.39 |
|
|
|
| 3 |
A' |
1077 |
1077 |
49.82 |
|
|
|
| 4 |
A' |
967 |
967 |
31.49 |
|
|
|
| 5 |
A' |
447 |
447 |
21.96 |
|
|
|
| 6 |
A" |
330 |
330 |
10.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4000.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4000.4 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.096 |
-1.284 |
0.000 |
| C2 |
0.000 |
0.093 |
0.000 |
| N3 |
-0.246 |
1.249 |
0.000 |
| H4 |
1.147 |
-1.601 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3804 | 2.5560 | 1.0978 |
C2 | 1.3804 | | 1.1819 | 2.0457 | N3 | 2.5560 | 1.1819 | | 3.1722 | H4 | 1.0978 | 2.0457 | 3.1722 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.131 |
|
|
|
| 2 |
C |
0.079 |
|
|
|
| 3 |
N |
-0.195 |
|
|
|
| 4 |
H |
0.246 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.834 |
-1.319 |
0.000 |
2.259 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.948 |
-2.423 |
0.000 |
| y |
-2.423 |
-21.411 |
0.000 |
| z |
0.000 |
0.000 |
-15.913 |
|
| Traceless |
| | x | y | z |
| x |
1.714 |
-2.423 |
0.000 |
| y |
-2.423 |
-4.981 |
0.000 |
| z |
0.000 |
0.000 |
3.267 |
|
| Polar |
| 3z2-r2 | 6.534 |
| x2-y2 | 4.464 |
| xy | -2.423 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.615 |
-0.747 |
0.000 |
| y |
-0.747 |
6.205 |
0.000 |
| z |
0.000 |
0.000 |
2.389 |
<r2> (average value of r
2) Å
2
| <r2> |
36.521 |
| (<r2>)1/2 |
6.043 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -131.301786 |
| Energy at 298.15K | -131.301244 |
| HF Energy | -131.163325 |
| Nuclear repulsion energy | 46.912737 |
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/6-311G*
Geometric Data calculated at B2PLYP/6-311G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability