Jump to
S1C2
Energy calculated at wB97X-D/6-31G*
| | hartrees |
| Energy at 0K | -131.365891 |
| Energy at 298.15K | -131.365215 |
| HF Energy | -131.365891 |
| Nuclear repulsion energy | |
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/6-31G*
| 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' |
3400 |
3225 |
30.74 |
|
|
|
| 2 |
A' |
1834 |
1739 |
29.96 |
|
|
|
| 3 |
A' |
1228 |
1165 |
9.43 |
|
|
|
| 4 |
A' |
502 |
476 |
31.57 |
|
|
|
| 5 |
A' |
384 |
364 |
19.09 |
|
|
|
| 6 |
A" |
448 |
425 |
2.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3897.9 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 3697.2 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 wB97X-D/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.194 |
-1.218 |
0.000 |
| C2 |
0.000 |
0.090 |
0.000 |
| N3 |
0.125 |
1.279 |
0.000 |
| H4 |
0.291 |
-2.179 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3225 | 2.5173 | 1.0762 |
C2 | 1.3225 | | 1.1954 | 2.2875 | N3 | 2.5173 | 1.1954 | | 3.4618 | H4 | 1.0762 | 2.2875 | 3.4618 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
177.551 |
|
C2 |
C1 |
H4 |
144.773 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.194 |
|
|
|
| 2 |
C |
0.364 |
|
|
|
| 3 |
N |
-0.426 |
|
|
|
| 4 |
H |
0.255 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.833 |
-3.045 |
0.000 |
3.157 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.341 |
-1.209 |
0.000 |
| y |
-1.209 |
-16.294 |
0.000 |
| z |
0.000 |
0.000 |
-16.938 |
|
| Traceless |
| | x | y | z |
| x |
0.275 |
-1.209 |
0.000 |
| y |
-1.209 |
0.346 |
0.000 |
| z |
0.000 |
0.000 |
-0.621 |
|
| Polar |
| 3z2-r2 | -1.242 |
| x2-y2 | -0.047 |
| xy | -1.209 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.804 |
-0.490 |
0.000 |
| y |
-0.490 |
6.091 |
0.000 |
| z |
0.000 |
0.000 |
1.625 |
<r2> (average value of r
2) Å
2
| <r2> |
35.904 |
| (<r2>)1/2 |
5.992 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31G*
| | hartrees |
| Energy at 0K | -131.364983 |
| Energy at 298.15K | |
| HF Energy | -131.364983 |
| Nuclear repulsion energy | |
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/6-31G*
| 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 |
3467 |
3288 |
63.15 |
|
|
|
| 2 |
Σ |
1732 |
1643 |
37.55 |
|
|
|
| 3 |
Σ |
1282 |
1216 |
6.87 |
|
|
|
| 4 |
Π |
449 |
425 |
0.85 |
|
|
|
| 4 |
Π |
449 |
425 |
0.85 |
|
|
|
| 5 |
Π |
330i |
313i |
55.23 |
|
|
|
| 5 |
Π |
330i |
313i |
55.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3358.9 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 3185.9 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 wB97X-D/6-31G*
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 |
0.089 |
| N3 |
0.000 |
0.000 |
1.289 |
| H4 |
0.000 |
0.000 |
-2.281 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3010 | 2.5014 | 1.0691 |
C2 | 1.3010 | | 1.2003 | 2.3701 | N3 | 2.5014 | 1.2003 | | 3.5704 | H4 | 1.0691 | 2.3701 | 3.5704 | |
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/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.132 |
|
|
|
| 2 |
C |
0.310 |
|
|
|
| 3 |
N |
-0.458 |
|
|
|
| 4 |
H |
0.280 |
|
|
|
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 |
-3.376 |
3.376 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.908 |
0.000 |
0.000 |
| y |
0.000 |
-16.908 |
0.000 |
| z |
0.000 |
0.000 |
-15.054 |
|
| Traceless |
| | x | y | z |
| x |
-0.927 |
0.000 |
0.000 |
| y |
0.000 |
-0.927 |
0.000 |
| z |
0.000 |
0.000 |
1.854 |
|
| Polar |
| 3z2-r2 | 3.707 |
| 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 |
1.630 |
0.000 |
0.000 |
| y |
0.000 |
1.630 |
0.000 |
| z |
0.000 |
0.000 |
6.158 |
<r2> (average value of r
2) Å
2
| <r2> |
35.872 |
| (<r2>)1/2 |
5.989 |