Jump to
S2C1
S3C1
Energy calculated at B97D3/6-31G*
| hartrees |
Energy at 0K | -55.185035 |
Energy at 298.15K | -55.184994 |
HF Energy | -55.185035 |
Nuclear repulsion energy | |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at B97D3/6-31G*
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.132 |
H2 |
0.000 |
0.000 |
-0.923 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.288 |
|
|
|
2 |
H |
0.288 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-1.553 |
1.553 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-6.135 |
0.000 |
0.000 |
y |
0.000 |
-6.135 |
0.000 |
z |
0.000 |
0.000 |
-5.790 |
|
Traceless |
| x | y | z |
x |
-0.172 |
0.000 |
0.000 |
y |
0.000 |
-0.172 |
0.000 |
z |
0.000 |
0.000 |
0.345 |
|
Polar |
3z2-r2 | 0.689 |
x2-y2 | 0.000 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.631 |
0.000 |
0.000 |
y |
0.000 |
0.631 |
0.000 |
z |
0.000 |
0.000 |
1.380 |
<r2> (average value of r
2) Å
2
<r2> |
4.734 |
(<r2>)1/2 |
2.176 |
Jump to
S1C1
S3C1
Energy calculated at B97D3/6-31G*
| hartrees |
Energy at 0K | -55.185035 |
Energy at 298.15K | -55.184994 |
HF Energy | -55.185035 |
Nuclear repulsion energy | |
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 B97D3/6-31G*
Geometric Data calculated at B97D3/6-31G*
Point Group is C∞v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
Energy calculated at B97D3/6-31G*
| hartrees |
Energy at 0K | -55.095080 |
Energy at 298.15K | -55.095040 |
HF Energy | -55.095080 |
Nuclear repulsion energy | |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at B97D3/6-31G*
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.132 |
H2 |
0.000 |
0.000 |
-0.922 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.298 |
|
|
|
2 |
H |
0.298 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-1.587 |
1.587 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-7.717 |
0.000 |
0.000 |
y |
0.000 |
-4.854 |
0.000 |
z |
0.000 |
0.000 |
-5.747 |
|
Traceless |
| x | y | z |
x |
-2.416 |
0.000 |
0.000 |
y |
0.000 |
1.878 |
0.000 |
z |
0.000 |
0.000 |
0.538 |
|
Polar |
3z2-r2 | 1.077 |
x2-y2 | -2.863 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.631 |
0.000 |
0.000 |
y |
0.000 |
0.631 |
0.000 |
z |
0.000 |
0.000 |
1.380 |
<r2> (average value of r
2) Å
2
<r2> |
4.784 |
(<r2>)1/2 |
2.187 |