Jump to
S1C2
Energy calculated at PBEPBE/3-21G*
| | hartrees |
| Energy at 0K | -93.316055 |
| Energy at 298.15K | -93.317332 |
| HF Energy | -93.316055 |
| Nuclear repulsion energy | 27.828281 |
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 PBEPBE/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' |
2997 |
2858 |
22.91 |
|
|
|
| 2 |
A' |
2848 |
2716 |
79.23 |
|
|
|
| 3 |
A' |
1807 |
1723 |
10.23 |
|
|
|
| 4 |
A' |
922 |
879 |
93.85 |
|
|
|
| 5 |
A' |
892 |
851 |
189.86 |
|
|
|
| 6 |
A" |
907 |
865 |
7.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5186.9 cm
-1
Scaled (by 0.9535) Zero Point Vibrational Energy (zpe) 4945.7 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 PBEPBE/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.107 |
0.648 |
0.000 |
| N2 |
0.107 |
-0.587 |
0.000 |
| H3 |
-0.667 |
1.444 |
0.000 |
| H4 |
-0.729 |
-1.225 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2349 | 1.1105 | 2.0512 |
N2 | 1.2349 | | 2.1733 | 1.0519 | H3 | 1.1105 | 2.1733 | | 2.6693 | H4 | 2.0512 | 1.0519 | 2.6693 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
127.339 |
|
H3 |
C1 |
N2 |
135.760 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.036 |
|
|
|
| 2 |
N |
-0.513 |
|
|
|
| 3 |
H |
0.194 |
|
|
|
| 4 |
H |
0.283 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.316 |
-0.036 |
0.000 |
2.316 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.176 |
0.580 |
0.000 |
| y |
0.580 |
-10.773 |
0.000 |
| z |
0.000 |
0.000 |
-12.385 |
|
| Traceless |
| | x | y | z |
| x |
-0.596 |
0.580 |
0.000 |
| y |
0.580 |
1.507 |
0.000 |
| z |
0.000 |
0.000 |
-0.911 |
|
| Polar |
| 3z2-r2 | -1.822 |
| x2-y2 | -1.402 |
| xy | 0.580 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.623 |
0.121 |
0.000 |
| y |
0.121 |
3.852 |
0.000 |
| z |
0.000 |
0.000 |
0.961 |
<r2> (average value of r
2) Å
2
| <r2> |
16.999 |
| (<r2>)1/2 |
4.123 |
Jump to
S1C1
Energy calculated at PBEPBE/3-21G*
| | hartrees |
| Energy at 0K | -93.323013 |
| Energy at 298.15K | -93.324354 |
| HF Energy | -93.323013 |
| Nuclear repulsion energy | 27.702487 |
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 PBEPBE/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' |
3199 |
3050 |
1.82 |
|
|
|
| 2 |
A' |
2921 |
2786 |
39.66 |
|
|
|
| 3 |
A' |
1714 |
1635 |
7.26 |
|
|
|
| 4 |
A' |
1180 |
1125 |
17.45 |
|
|
|
| 5 |
A' |
924 |
881 |
212.51 |
|
|
|
| 6 |
A" |
983 |
937 |
120.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5460.7 cm
-1
Scaled (by 0.9535) Zero Point Vibrational Energy (zpe) 5206.8 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 PBEPBE/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.002 |
0.663 |
0.000 |
| N2 |
-0.002 |
-0.590 |
0.000 |
| H3 |
0.923 |
1.275 |
0.000 |
| H4 |
-0.898 |
-1.123 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
H3 |
H4 |
| C1 | | 1.2527 | 1.1088 | 1.9980 |
N2 | 1.2527 | | 2.0814 | 1.0426 | H3 | 1.1088 | 2.0814 | | 3.0107 | H4 | 1.9980 | 1.0426 | 3.0107 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N2 |
H4 |
120.751 |
|
H3 |
C1 |
N2 |
123.506 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.014 |
|
|
|
| 2 |
N |
-0.501 |
|
|
|
| 3 |
H |
0.211 |
|
|
|
| 4 |
H |
0.303 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.504 |
-0.171 |
0.000 |
0.532 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.091 |
3.261 |
0.000 |
| y |
3.261 |
-11.387 |
0.000 |
| z |
0.000 |
0.000 |
-12.437 |
|
| Traceless |
| | x | y | z |
| x |
0.820 |
3.261 |
0.000 |
| y |
3.261 |
0.378 |
0.000 |
| z |
0.000 |
0.000 |
-1.198 |
|
| Polar |
| 3z2-r2 | -2.397 |
| x2-y2 | 0.295 |
| xy | 3.261 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.986 |
0.620 |
0.000 |
| y |
0.620 |
3.450 |
0.000 |
| z |
0.000 |
0.000 |
0.995 |
<r2> (average value of r
2) Å
2
| <r2> |
16.885 |
| (<r2>)1/2 |
4.109 |