Jump to
S1C2
Energy calculated at M06-2X/cc-pVTZ
| | hartrees |
| Energy at 0K | -93.950422 |
| Energy at 298.15K | -93.951723 |
| HF Energy | -93.950422 |
| Nuclear repulsion energy | 28.342730 |
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/cc-pVTZ
| 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' |
3342 |
3192 |
6.04 |
|
|
|
| 2 |
A' |
3030 |
2894 |
32.02 |
|
|
|
| 3 |
A' |
1884 |
1799 |
39.70 |
|
|
|
| 4 |
A' |
1039 |
993 |
135.59 |
|
|
|
| 5 |
A' |
854 |
816 |
115.56 |
|
|
|
| 6 |
A" |
928 |
887 |
3.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5538.8 cm
-1
Scaled (by 0.9551) Zero Point Vibrational Energy (zpe) 5290.1 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 M06-2X/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.112 |
0.633 |
0.000 |
| N2 |
0.112 |
-0.585 |
0.000 |
| H3 |
-0.675 |
1.395 |
0.000 |
| H4 |
-0.776 |
-1.098 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2180 | 1.0955 | 1.9454 |
N2 | 1.2180 | | 2.1307 | 1.0251 | H3 | 1.0955 | 2.1307 | | 2.4952 | H4 | 1.9454 | 1.0251 | 2.4952 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
120.047 |
|
H3 |
C1 |
N2 |
134.072 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.092 |
|
|
|
| 2 |
N |
-0.221 |
|
|
|
| 3 |
H |
0.122 |
|
|
|
| 4 |
H |
0.192 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.151 |
0.481 |
0.000 |
2.204 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.176 |
0.658 |
0.000 |
| y |
0.658 |
-11.190 |
0.000 |
| z |
0.000 |
0.000 |
-12.774 |
|
| Traceless |
| | x | y | z |
| x |
-0.194 |
0.658 |
0.000 |
| y |
0.658 |
1.286 |
0.000 |
| z |
0.000 |
0.000 |
-1.091 |
|
| Polar |
| 3z2-r2 | -2.183 |
| x2-y2 | -0.987 |
| xy | 0.658 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.490 |
0.107 |
0.000 |
| y |
0.107 |
4.099 |
0.000 |
| z |
0.000 |
0.000 |
1.817 |
<r2> (average value of r
2) Å
2
| <r2> |
16.696 |
| (<r2>)1/2 |
4.086 |
Jump to
S1C1
Energy calculated at M06-2X/cc-pVTZ
| | hartrees |
| Energy at 0K | -93.957119 |
| Energy at 298.15K | -93.958462 |
| HF Energy | -93.957119 |
| Nuclear repulsion energy | 28.293189 |
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/cc-pVTZ
| 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' |
3439 |
3285 |
16.02 |
|
|
|
| 2 |
A' |
3045 |
2908 |
20.38 |
|
|
|
| 3 |
A' |
1849 |
1766 |
37.58 |
|
|
|
| 4 |
A' |
1192 |
1138 |
9.24 |
|
|
|
| 5 |
A' |
896 |
855 |
251.90 |
|
|
|
| 6 |
A" |
987 |
943 |
112.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5703.4 cm
-1
Scaled (by 0.9551) Zero Point Vibrational Energy (zpe) 5447.3 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.644 |
0.000 |
| N2 |
0.000 |
-0.581 |
0.000 |
| H3 |
0.896 |
1.274 |
0.000 |
| H4 |
-0.897 |
-1.067 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2251 | 1.0952 | 1.9315 |
N2 | 1.2251 | | 2.0605 | 1.0202 | H3 | 1.0952 | 2.0605 | | 2.9486 | H4 | 1.9315 | 1.0202 | 2.9486 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.401 |
|
H3 |
C1 |
N2 |
125.161 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.123 |
|
|
|
| 2 |
N |
-0.230 |
|
|
|
| 3 |
H |
0.144 |
|
|
|
| 4 |
H |
0.210 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.450 |
0.210 |
0.000 |
0.497 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.377 |
3.152 |
0.000 |
| y |
3.152 |
-11.462 |
0.000 |
| z |
0.000 |
0.000 |
-12.806 |
|
| Traceless |
| | x | y | z |
| x |
0.758 |
3.152 |
0.000 |
| y |
3.152 |
0.629 |
0.000 |
| z |
0.000 |
0.000 |
-1.387 |
|
| Polar |
| 3z2-r2 | -2.774 |
| x2-y2 | 0.086 |
| xy | 3.152 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.660 |
0.308 |
0.000 |
| y |
0.308 |
4.000 |
0.000 |
| z |
0.000 |
0.000 |
1.858 |
<r2> (average value of r
2) Å
2
| <r2> |
16.642 |
| (<r2>)1/2 |
4.079 |