Jump to
S1C2
Energy calculated at M06-2X/3-21G*
| | hartrees |
| Energy at 0K | -93.379853 |
| Energy at 298.15K | -93.381146 |
| HF Energy | -93.379853 |
| Nuclear repulsion energy | 28.112554 |
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/3-21G*
| 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' |
3209 |
3040 |
1.06 |
|
|
|
| 2 |
A' |
2977 |
2820 |
35.08 |
|
|
|
| 3 |
A' |
1912 |
1811 |
21.43 |
|
|
|
| 4 |
A' |
1004 |
951 |
61.97 |
|
|
|
| 5 |
A' |
842 |
798 |
265.10 |
|
|
|
| 6 |
A" |
958 |
908 |
12.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5450.8 cm
-1
Scaled (by 0.9472) Zero Point Vibrational Energy (zpe) 5163.0 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 M06-2X/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.105 |
0.644 |
0.000 |
| N2 |
0.105 |
-0.580 |
0.000 |
| H3 |
-0.667 |
1.425 |
0.000 |
| H4 |
-0.698 |
-1.233 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2236 | 1.0986 | 2.0413 |
N2 | 1.2236 | | 2.1484 | 1.0349 | H3 | 1.0986 | 2.1484 | | 2.6581 | H4 | 2.0413 | 1.0349 | 2.6581 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
129.137 |
|
H3 |
C1 |
N2 |
135.318 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.052 |
|
|
|
| 2 |
N |
-0.554 |
|
|
|
| 3 |
H |
0.196 |
|
|
|
| 4 |
H |
0.306 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.444 |
0.039 |
0.000 |
2.444 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.244 |
0.708 |
0.000 |
| y |
0.708 |
-10.617 |
0.000 |
| z |
0.000 |
0.000 |
-12.431 |
|
| Traceless |
| | x | y | z |
| x |
-0.720 |
0.708 |
0.000 |
| y |
0.708 |
1.720 |
0.000 |
| z |
0.000 |
0.000 |
-1.000 |
|
| Polar |
| 3z2-r2 | -2.000 |
| x2-y2 | -1.627 |
| xy | 0.708 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.496 |
0.095 |
0.000 |
| y |
0.095 |
3.697 |
0.000 |
| z |
0.000 |
0.000 |
0.935 |
<r2> (average value of r
2) Å
2
| <r2> |
16.814 |
| (<r2>)1/2 |
4.100 |
Jump to
S1C1
Energy calculated at M06-2X/3-21G*
| | hartrees |
| Energy at 0K | -93.386630 |
| Energy at 298.15K | -93.387985 |
| HF Energy | -93.386630 |
| Nuclear repulsion energy | 28.005815 |
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/3-21G*
| 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' |
3395 |
3215 |
7.00 |
|
|
|
| 2 |
A' |
3104 |
2940 |
22.43 |
|
|
|
| 3 |
A' |
1821 |
1725 |
16.30 |
|
|
|
| 4 |
A' |
1213 |
1149 |
9.13 |
|
|
|
| 5 |
A' |
938 |
888 |
264.81 |
|
|
|
| 6 |
A" |
1020 |
966 |
139.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5745.3 cm
-1
Scaled (by 0.9472) Zero Point Vibrational Energy (zpe) 5441.9 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 M06-2X/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.656 |
0.000 |
| N2 |
-0.002 |
-0.582 |
0.000 |
| H3 |
0.897 |
1.282 |
0.000 |
| H4 |
-0.869 |
-1.140 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2378 | 1.0962 | 1.9936 |
N2 | 1.2378 | | 2.0701 | 1.0303 | H3 | 1.0962 | 2.0701 | | 2.9975 | H4 | 1.9936 | 1.0303 | 2.9975 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
122.773 |
|
H3 |
C1 |
N2 |
124.872 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.011 |
|
|
|
| 2 |
N |
-0.545 |
|
|
|
| 3 |
H |
0.215 |
|
|
|
| 4 |
H |
0.319 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.566 |
-0.031 |
0.000 |
0.567 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.193 |
3.382 |
0.000 |
| y |
3.382 |
-11.203 |
0.000 |
| z |
0.000 |
0.000 |
-12.477 |
|
| Traceless |
| | x | y | z |
| x |
0.646 |
3.382 |
0.000 |
| y |
3.382 |
0.632 |
0.000 |
| z |
0.000 |
0.000 |
-1.278 |
|
| Polar |
| 3z2-r2 | -2.557 |
| x2-y2 | 0.010 |
| xy | 3.382 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.885 |
0.493 |
0.000 |
| y |
0.493 |
3.426 |
0.000 |
| z |
0.000 |
0.000 |
0.970 |
<r2> (average value of r
2) Å
2
| <r2> |
16.715 |
| (<r2>)1/2 |
4.088 |