Jump to
S1C2
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -93.933011 |
| Energy at 298.15K | -93.934315 |
| HF Energy | -93.933011 |
| Nuclear repulsion energy | 28.287723 |
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/6-311G*
| 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' |
3337 |
3337 |
1.88 |
|
|
|
| 2 |
A' |
3032 |
3032 |
41.75 |
|
|
|
| 3 |
A' |
1887 |
1887 |
38.58 |
|
|
|
| 4 |
A' |
1053 |
1053 |
133.83 |
|
|
|
| 5 |
A' |
868 |
868 |
126.54 |
|
|
|
| 6 |
A" |
932 |
932 |
5.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5554.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5554.3 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.112 |
0.634 |
0.000 |
| N2 |
0.112 |
-0.586 |
0.000 |
| H3 |
-0.679 |
1.396 |
0.000 |
| H4 |
-0.778 |
-1.098 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2205 | 1.0978 | 1.9477 |
N2 | 1.2205 | | 2.1339 | 1.0269 | H3 | 1.0978 | 2.1339 | | 2.4956 | H4 | 1.9477 | 1.0269 | 2.4956 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
119.893 |
|
H3 |
C1 |
N2 |
133.911 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.067 |
|
|
|
| 2 |
N |
-0.473 |
|
|
|
| 3 |
H |
0.223 |
|
|
|
| 4 |
H |
0.317 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.346 |
0.507 |
0.000 |
2.400 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.077 |
0.728 |
0.000 |
| y |
0.728 |
-11.224 |
0.000 |
| z |
0.000 |
0.000 |
-12.733 |
|
| Traceless |
| | x | y | z |
| x |
-0.098 |
0.728 |
0.000 |
| y |
0.728 |
1.181 |
0.000 |
| z |
0.000 |
0.000 |
-1.082 |
|
| Polar |
| 3z2-r2 | -2.165 |
| x2-y2 | -0.853 |
| xy | 0.728 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.090 |
0.121 |
0.000 |
| y |
0.121 |
3.874 |
0.000 |
| z |
0.000 |
0.000 |
1.383 |
<r2> (average value of r
2) Å
2
| <r2> |
16.705 |
| (<r2>)1/2 |
4.087 |
Jump to
S1C1
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -93.940815 |
| Energy at 298.15K | -93.942165 |
| HF Energy | -93.940815 |
| Nuclear repulsion energy | 28.240814 |
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/6-311G*
| 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' |
3450 |
3450 |
6.95 |
|
|
|
| 2 |
A' |
3071 |
3071 |
24.99 |
|
|
|
| 3 |
A' |
1853 |
1853 |
37.07 |
|
|
|
| 4 |
A' |
1226 |
1226 |
11.57 |
|
|
|
| 5 |
A' |
918 |
918 |
263.93 |
|
|
|
| 6 |
A" |
1000 |
1000 |
131.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5759.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5759.1 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.001 |
0.646 |
0.000 |
| N2 |
-0.001 |
-0.582 |
0.000 |
| H3 |
0.905 |
1.265 |
0.000 |
| H4 |
-0.899 |
-1.068 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2280 | 1.0969 | 1.9352 |
N2 | 1.2280 | | 2.0568 | 1.0213 | H3 | 1.0969 | 2.0568 | | 2.9489 | H4 | 1.9352 | 1.0213 | 2.9489 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
118.419 |
|
H3 |
C1 |
N2 |
124.324 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.103 |
|
|
|
| 2 |
N |
-0.465 |
|
|
|
| 3 |
H |
0.236 |
|
|
|
| 4 |
H |
0.332 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.539 |
0.203 |
0.000 |
0.576 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.214 |
3.281 |
0.000 |
| y |
3.281 |
-11.498 |
0.000 |
| z |
0.000 |
0.000 |
-12.763 |
|
| Traceless |
| | x | y | z |
| x |
0.917 |
3.281 |
0.000 |
| y |
3.281 |
0.491 |
0.000 |
| z |
0.000 |
0.000 |
-1.407 |
|
| Polar |
| 3z2-r2 | -2.815 |
| x2-y2 | 0.284 |
| xy | 3.281 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.310 |
0.330 |
0.000 |
| y |
0.330 |
3.792 |
0.000 |
| z |
0.000 |
0.000 |
1.450 |
<r2> (average value of r
2) Å
2
| <r2> |
16.628 |
| (<r2>)1/2 |
4.078 |