Jump to
S1C2
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -131.398883 |
| Energy at 298.15K | -131.398157 |
| HF Energy | -131.398883 |
| Nuclear repulsion energy | 47.529585 |
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 wB97X-D/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' |
3389 |
3241 |
40.64 |
|
|
|
| 2 |
A' |
1790 |
1712 |
35.45 |
|
|
|
| 3 |
A' |
1228 |
1175 |
10.13 |
|
|
|
| 4 |
A' |
466 |
446 |
9.80 |
|
|
|
| 5 |
A' |
348 |
333 |
39.85 |
|
|
|
| 6 |
A" |
453 |
433 |
1.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3836.9 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 3670.0 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 wB97X-D/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.204 |
-1.210 |
0.000 |
| C2 |
0.000 |
0.090 |
0.000 |
| N3 |
0.137 |
1.271 |
0.000 |
| H4 |
0.264 |
-2.177 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3168 | 2.5049 | 1.0741 |
C2 | 1.3168 | | 1.1886 | 2.2830 | N3 | 2.5049 | 1.1886 | | 3.4506 | H4 | 1.0741 | 2.2830 | 3.4506 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
177.715 |
|
C2 |
C1 |
H4 |
145.244 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.048 |
|
|
|
| 2 |
C |
0.077 |
|
|
|
| 3 |
N |
-0.227 |
|
|
|
| 4 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.757 |
-3.093 |
0.000 |
3.184 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.754 |
-1.100 |
0.000 |
| y |
-1.100 |
-16.265 |
0.000 |
| z |
0.000 |
0.000 |
-17.217 |
|
| Traceless |
| | x | y | z |
| x |
-0.013 |
-1.100 |
0.000 |
| y |
-1.100 |
0.720 |
0.000 |
| z |
0.000 |
0.000 |
-0.707 |
|
| Polar |
| 3z2-r2 | -1.414 |
| x2-y2 | -0.488 |
| xy | -1.100 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.025 |
-0.414 |
0.000 |
| y |
-0.414 |
6.350 |
0.000 |
| z |
0.000 |
0.000 |
1.919 |
<r2> (average value of r
2) Å
2
| <r2> |
35.843 |
| (<r2>)1/2 |
5.987 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -131.398496 |
| Energy at 298.15K | |
| HF Energy | -131.398496 |
| Nuclear repulsion energy | 47.595496 |
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 wB97X-D/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 |
3439 |
3289 |
67.07 |
|
|
|
| 2 |
Σ |
1713 |
1639 |
40.79 |
|
|
|
| 3 |
Σ |
1270 |
1215 |
7.62 |
|
|
|
| 4 |
Π |
452 |
433 |
0.46 |
|
|
|
| 4 |
Π |
452 |
433 |
0.46 |
|
|
|
| 5 |
Π |
265i |
254i |
50.65 |
|
|
|
| 5 |
Π |
265i |
254i |
50.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3398.3 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 3250.5 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 wB97X-D/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.206 |
| C2 |
0.000 |
0.000 |
0.089 |
| N3 |
0.000 |
0.000 |
1.282 |
| H4 |
0.000 |
0.000 |
-2.273 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2955 | 2.4889 | 1.0662 |
C2 | 1.2955 | | 1.1935 | 2.3617 | N3 | 2.4889 | 1.1935 | | 3.5552 | H4 | 1.0662 | 2.3617 | 3.5552 | |
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 wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.002 |
|
|
|
| 2 |
C |
0.044 |
|
|
|
| 3 |
N |
-0.228 |
|
|
|
| 4 |
H |
0.182 |
|
|
|
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 |
-3.323 |
3.323 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.198 |
0.000 |
0.000 |
| y |
0.000 |
-17.198 |
0.000 |
| z |
0.000 |
0.000 |
-15.373 |
|
| Traceless |
| | x | y | z |
| x |
-0.913 |
0.000 |
0.000 |
| y |
0.000 |
-0.913 |
0.000 |
| z |
0.000 |
0.000 |
1.825 |
|
| Polar |
| 3z2-r2 | 3.650 |
| 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 |
1.918 |
0.000 |
0.000 |
| y |
0.000 |
1.918 |
0.000 |
| z |
0.000 |
0.000 |
6.401 |
<r2> (average value of r
2) Å
2
| <r2> |
35.812 |
| (<r2>)1/2 |
5.984 |