Jump to
S2C1
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -25.126248 |
| Energy at 298.15K | -25.125022 |
| HF Energy | -25.126248 |
| Nuclear repulsion energy | 2.156660 |
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 HF/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| B1 |
0.000 |
0.000 |
0.204 |
| H2 |
0.000 |
0.000 |
-1.022 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.031 |
|
|
|
| 2 |
H |
0.031 |
|
|
|
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 |
-1.696 |
1.696 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.000 |
0.000 |
-1.362 |
1.362 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.569 |
0.000 |
0.000 |
| y |
0.000 |
-6.569 |
0.000 |
| z |
0.000 |
0.000 |
-10.734 |
|
| Traceless |
| | x | y | z |
| x |
2.083 |
0.000 |
0.000 |
| y |
0.000 |
2.083 |
0.000 |
| z |
0.000 |
0.000 |
-4.165 |
|
| Polar |
| 3z2-r2 | -8.331 |
| 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 |
2.691 |
0.000 |
0.000 |
| y |
0.000 |
2.691 |
0.000 |
| z |
0.000 |
0.000 |
3.080 |
<r2> (average value of r
2) Å
2
| <r2> |
6.224 |
| (<r2>)1/2 |
2.495 |
Jump to
S1C1
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -25.112760 |
| Energy at 298.15K | -25.111533 |
| HF Energy | -25.112760 |
| Nuclear repulsion energy | 2.237930 |
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 HF/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| B1 |
0.000 |
0.000 |
0.197 |
| H2 |
0.000 |
0.000 |
-0.985 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.116 |
|
|
|
| 2 |
H |
0.116 |
|
|
|
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 |
-0.106 |
0.106 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-5.961 |
0.000 |
0.000 |
| y |
0.000 |
-9.240 |
0.000 |
| z |
0.000 |
0.000 |
-7.576 |
|
| Traceless |
| | x | y | z |
| x |
2.447 |
0.000 |
0.000 |
| y |
0.000 |
-2.471 |
0.000 |
| z |
0.000 |
0.000 |
0.024 |
|
| Polar |
| 3z2-r2 | 0.048 |
| x2-y2 | 3.279 |
| 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 |
1.693 |
0.000 |
0.000 |
| y |
0.000 |
1.483 |
0.000 |
| z |
0.000 |
0.000 |
1.967 |
<r2> (average value of r
2) Å
2
| <r2> |
5.907 |
| (<r2>)1/2 |
2.430 |