Jump to
S1C2
Energy calculated at PBE1PBE/6-311G*
| | hartrees |
| Energy at 0K | -90.478902 |
| Energy at 298.15K | -90.478681 |
| HF Energy | -90.478902 |
| Nuclear repulsion energy | 17.569293 |
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/6-311G*
| 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' |
4068 |
3899 |
126.09 |
93.12 |
0.27 |
0.42 |
| 2 |
A' |
1295 |
1241 |
99.92 |
5.34 |
0.71 |
0.83 |
| 3 |
A' |
319 |
306 |
215.38 |
11.29 |
0.60 |
0.75 |
Unscaled Zero Point Vibrational Energy (zpe) 2841.3 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 2723.4 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.042 |
-0.369 |
0.000 |
| Be2 |
0.042 |
1.024 |
0.000 |
| H3 |
-0.506 |
-1.143 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
Be2 |
H3 |
| O1 | | 1.3929 | 0.9482 |
Be2 | 1.3929 | | 2.2347 | H3 | 0.9482 | 2.2347 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be2 |
O1 |
H3 |
144.655 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.735 |
|
|
|
| 2 |
Be |
0.299 |
|
|
|
| 3 |
H |
0.436 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.095 |
-1.012 |
0.000 |
1.491 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.244 |
1.568 |
0.000 |
| y |
1.568 |
-11.897 |
0.000 |
| z |
0.000 |
0.000 |
-12.056 |
|
| Traceless |
| | x | y | z |
| x |
0.733 |
1.568 |
0.000 |
| y |
1.568 |
-0.247 |
0.000 |
| z |
0.000 |
0.000 |
-0.486 |
|
| Polar |
| 3z2-r2 | -0.972 |
| x2-y2 | 0.653 |
| xy | 1.568 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.553 |
0.164 |
0.000 |
| y |
0.164 |
3.893 |
0.000 |
| z |
0.000 |
0.000 |
4.330 |
<r2> (average value of r
2) Å
2
| <r2> |
14.193 |
| (<r2>)1/2 |
3.767 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-311G*
| | hartrees |
| Energy at 0K | -90.478402 |
| Energy at 298.15K | |
| HF Energy | -90.478402 |
| Nuclear repulsion energy | 17.708596 |
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/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
4141 |
3969 |
181.08 |
|
|
|
| 2 |
Σ |
1335 |
1279 |
116.44 |
|
|
|
| 3 |
Π |
225i |
215i |
198.85 |
|
|
|
| 3 |
Π |
225i |
215i |
198.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2513.2 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 2408.9 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 PBE1PBE/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
0.351 |
| Be2 |
0.000 |
0.000 |
-1.025 |
| H3 |
0.000 |
0.000 |
1.294 |
Atom - Atom Distances (Å)
| |
O1 |
Be2 |
H3 |
| O1 | | 1.3756 | 0.9436 |
Be2 | 1.3756 | | 2.3193 | H3 | 0.9436 | 2.3193 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be2 |
O1 |
H3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.743 |
|
|
|
| 2 |
Be |
0.305 |
|
|
|
| 3 |
H |
0.437 |
|
|
|
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 |
1.554 |
1.554 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.023 |
0.000 |
0.000 |
| y |
0.000 |
-12.023 |
0.000 |
| z |
0.000 |
0.000 |
-10.899 |
|
| Traceless |
| | x | y | z |
| x |
-0.562 |
0.000 |
0.000 |
| y |
0.000 |
-0.562 |
0.000 |
| z |
0.000 |
0.000 |
1.124 |
|
| Polar |
| 3z2-r2 | 2.248 |
| 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 |
4.334 |
0.000 |
0.000 |
| y |
0.000 |
4.334 |
0.000 |
| z |
0.000 |
0.000 |
3.962 |
<r2> (average value of r
2) Å
2
| <r2> |
14.137 |
| (<r2>)1/2 |
3.760 |