Jump to
S1C2
Energy calculated at M06-2X/6-31G**
| | hartrees |
| Energy at 0K | -93.910942 |
| Energy at 298.15K | -93.912237 |
| HF Energy | -93.910942 |
| Nuclear repulsion energy | 28.201261 |
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 M06-2X/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' |
3349 |
3183 |
2.42 |
|
|
|
| 2 |
A' |
3048 |
2897 |
48.66 |
|
|
|
| 3 |
A' |
1899 |
1805 |
37.93 |
|
|
|
| 4 |
A' |
1045 |
994 |
121.98 |
|
|
|
| 5 |
A' |
849 |
807 |
144.65 |
|
|
|
| 6 |
A" |
925 |
879 |
5.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5557.3 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 5281.7 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 M06-2X/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.112 |
0.636 |
0.000 |
| N2 |
0.112 |
-0.589 |
0.000 |
| H3 |
-0.674 |
1.404 |
0.000 |
| H4 |
-0.782 |
-1.097 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2252 | 1.0993 | 1.9497 |
N2 | 1.2252 | | 2.1430 | 1.0277 | H3 | 1.0993 | 2.1430 | | 2.5035 | H4 | 1.9497 | 1.0277 | 2.5035 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
119.602 |
|
H3 |
C1 |
N2 |
134.341 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.052 |
|
|
|
| 2 |
N |
-0.462 |
|
|
|
| 3 |
H |
0.134 |
|
|
|
| 4 |
H |
0.275 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.211 |
0.525 |
0.000 |
2.273 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.852 |
0.800 |
0.000 |
| y |
0.800 |
-10.998 |
0.000 |
| z |
0.000 |
0.000 |
-12.450 |
|
| Traceless |
| | x | y | z |
| x |
-0.128 |
0.800 |
0.000 |
| y |
0.800 |
1.154 |
0.000 |
| z |
0.000 |
0.000 |
-1.025 |
|
| Polar |
| 3z2-r2 | -2.050 |
| x2-y2 | -0.855 |
| xy | 0.800 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.974 |
0.077 |
0.000 |
| y |
0.077 |
3.825 |
0.000 |
| z |
0.000 |
0.000 |
1.198 |
<r2> (average value of r
2) Å
2
| <r2> |
16.610 |
| (<r2>)1/2 |
4.076 |
Jump to
S1C1
Energy calculated at M06-2X/6-31G**
| | hartrees |
| Energy at 0K | -93.918585 |
| Energy at 298.15K | -93.919927 |
| HF Energy | -93.918585 |
| Nuclear repulsion energy | 28.158749 |
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 M06-2X/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' |
3462 |
3291 |
7.88 |
|
|
|
| 2 |
A' |
3059 |
2907 |
30.04 |
|
|
|
| 3 |
A' |
1867 |
1774 |
35.48 |
|
|
|
| 4 |
A' |
1210 |
1150 |
8.57 |
|
|
|
| 5 |
A' |
900 |
855 |
254.20 |
|
|
|
| 6 |
A" |
992 |
942 |
117.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5744.7 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 5459.7 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 M06-2X/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.648 |
0.000 |
| N2 |
-0.000 |
-0.585 |
0.000 |
| H3 |
0.906 |
1.270 |
0.000 |
| H4 |
-0.903 |
-1.065 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2325 | 1.0990 | 1.9360 |
N2 | 1.2325 | | 2.0641 | 1.0225 | H3 | 1.0990 | 2.0641 | | 2.9535 | H4 | 1.9360 | 1.0225 | 2.9535 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.012 |
|
H3 |
C1 |
N2 |
124.482 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.012 |
|
|
|
| 2 |
N |
-0.450 |
|
|
|
| 3 |
H |
0.146 |
|
|
|
| 4 |
H |
0.293 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.577 |
0.229 |
0.000 |
0.621 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.042 |
3.084 |
0.000 |
| y |
3.084 |
-11.286 |
0.000 |
| z |
0.000 |
0.000 |
-12.478 |
|
| Traceless |
| | x | y | z |
| x |
0.840 |
3.084 |
0.000 |
| y |
3.084 |
0.474 |
0.000 |
| z |
0.000 |
0.000 |
-1.314 |
|
| Polar |
| 3z2-r2 | -2.628 |
| x2-y2 | 0.244 |
| xy | 3.084 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.220 |
0.477 |
0.000 |
| y |
0.477 |
3.696 |
0.000 |
| z |
0.000 |
0.000 |
1.243 |
<r2> (average value of r
2) Å
2
| <r2> |
16.540 |
| (<r2>)1/2 |
4.067 |