Jump to
S1C2
Energy calculated at PBE1PBE/6-31G*
| | hartrees |
| Energy at 0K | -93.840730 |
| Energy at 298.15K | -93.842029 |
| HF Energy | -93.840730 |
| Nuclear repulsion energy | 28.176274 |
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 PBE1PBE/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' |
3339 |
3174 |
4.03 |
|
|
|
| 2 |
A' |
3027 |
2876 |
57.86 |
|
|
|
| 3 |
A' |
1890 |
1796 |
28.62 |
|
|
|
| 4 |
A' |
1038 |
986 |
134.39 |
|
|
|
| 5 |
A' |
885 |
841 |
121.92 |
|
|
|
| 6 |
A" |
920 |
875 |
6.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5549.5 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 5273.7 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 PBE1PBE/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.111 |
0.637 |
0.000 |
| N2 |
0.111 |
-0.589 |
0.000 |
| H3 |
-0.674 |
1.408 |
0.000 |
| H4 |
-0.775 |
-1.110 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2258 | 1.1007 | 1.9588 |
N2 | 1.2258 | | 2.1458 | 1.0282 | H3 | 1.1007 | 2.1458 | | 2.5200 | H4 | 1.9588 | 1.0282 | 2.5200 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
120.448 |
|
H3 |
C1 |
N2 |
134.472 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.013 |
|
|
|
| 2 |
N |
-0.498 |
|
|
|
| 3 |
H |
0.176 |
|
|
|
| 4 |
H |
0.334 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.236 |
0.456 |
0.000 |
2.282 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.859 |
0.770 |
0.000 |
| y |
0.770 |
-10.926 |
0.000 |
| z |
0.000 |
0.000 |
-12.422 |
|
| Traceless |
| | x | y | z |
| x |
-0.185 |
0.770 |
0.000 |
| y |
0.770 |
1.215 |
0.000 |
| z |
0.000 |
0.000 |
-1.029 |
|
| Polar |
| 3z2-r2 | -2.059 |
| x2-y2 | -0.933 |
| xy | 0.770 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.924 |
0.045 |
0.000 |
| y |
0.045 |
3.784 |
0.000 |
| z |
0.000 |
0.000 |
1.183 |
<r2> (average value of r
2) Å
2
| <r2> |
16.622 |
| (<r2>)1/2 |
4.077 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-31G*
| | hartrees |
| Energy at 0K | -93.848909 |
| Energy at 298.15K | -93.850256 |
| HF Energy | -93.848909 |
| Nuclear repulsion energy | 28.114654 |
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 PBE1PBE/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' |
3467 |
3295 |
2.99 |
|
|
|
| 2 |
A' |
3076 |
2923 |
32.56 |
|
|
|
| 3 |
A' |
1843 |
1751 |
28.67 |
|
|
|
| 4 |
A' |
1227 |
1166 |
11.95 |
|
|
|
| 5 |
A' |
927 |
881 |
224.12 |
|
|
|
| 6 |
A" |
993 |
944 |
116.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5766.4 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 5479.8 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 PBE1PBE/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
0.649 |
0.000 |
| N2 |
-0.000 |
-0.586 |
0.000 |
| H3 |
0.908 |
1.268 |
0.000 |
| H4 |
-0.906 |
-1.062 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2355 | 1.0990 | 1.9358 |
N2 | 1.2355 | | 2.0645 | 1.0226 | H3 | 1.0990 | 2.0645 | | 2.9523 | H4 | 1.9358 | 1.0226 | 2.9523 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
117.713 |
|
H3 |
C1 |
N2 |
124.237 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.050 |
|
|
|
| 2 |
N |
-0.487 |
|
|
|
| 3 |
H |
0.189 |
|
|
|
| 4 |
H |
0.348 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.583 |
0.231 |
0.000 |
0.627 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.998 |
3.096 |
0.000 |
| y |
3.096 |
-11.300 |
0.000 |
| z |
0.000 |
0.000 |
-12.454 |
|
| Traceless |
| | x | y | z |
| x |
0.878 |
3.096 |
0.000 |
| y |
3.096 |
0.427 |
0.000 |
| z |
0.000 |
0.000 |
-1.305 |
|
| Polar |
| 3z2-r2 | -2.611 |
| x2-y2 | 0.301 |
| xy | 3.096 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.161 |
0.508 |
0.000 |
| y |
0.508 |
3.611 |
0.000 |
| z |
0.000 |
0.000 |
1.229 |
<r2> (average value of r
2) Å
2
| <r2> |
16.549 |
| (<r2>)1/2 |
4.068 |