Jump to
S1C2
Energy calculated at B2PLYP=FULL/Def2TZVPP
| | hartrees |
| Energy at 0K | -166.498536 |
| Energy at 298.15K | |
| HF Energy | -166.308291 |
| Nuclear repulsion energy | 48.928200 |
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 B2PLYP=FULL/Def2TZVPP
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
4015 |
4015 |
49.52 |
|
|
|
| 2 |
A1 |
742 |
742 |
5.49 |
|
|
|
| 3 |
A1 |
584 |
584 |
173.07 |
|
|
|
| 4 |
A1 |
297 |
297 |
9.24 |
|
|
|
| 5 |
A2 |
209i |
209i |
0.00 |
|
|
|
| 6 |
B1 |
344 |
344 |
52.97 |
|
|
|
| 7 |
B2 |
4012 |
4012 |
177.80 |
|
|
|
| 8 |
B2 |
1528 |
1528 |
396.99 |
|
|
|
| 9 |
B2 |
477 |
477 |
275.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5894.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5894.8 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 B2PLYP=FULL/Def2TZVPP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
-0.011 |
| O2 |
0.000 |
1.426 |
0.078 |
| O3 |
0.000 |
-1.426 |
0.078 |
| H4 |
0.000 |
2.090 |
-0.602 |
| H5 |
0.000 |
-2.090 |
-0.602 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.4288 | 1.4288 | 2.1717 | 2.1717 |
O2 | 1.4288 | | 2.8520 | 0.9503 | 3.5809 | O3 | 1.4288 | 2.8520 | | 3.5809 | 0.9503 | H4 | 2.1717 | 0.9503 | 3.5809 | | 4.1794 | H5 | 2.1717 | 3.5809 | 0.9503 | 4.1794 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
130.727 |
|
Be1 |
O3 |
H5 |
130.727 |
| O2 |
Be1 |
O3 |
172.858 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/Def2TZVPP
| | hartrees |
| Energy at 0K | -166.499309 |
| Energy at 298.15K | -166.500774 |
| HF Energy | -166.309005 |
| Nuclear repulsion energy | 48.910998 |
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 B2PLYP=FULL/Def2TZVPP
| 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 |
4000 |
4000 |
22.82 |
|
|
|
| 2 |
A |
738 |
738 |
1.59 |
|
|
|
| 3 |
A |
576 |
576 |
86.83 |
|
|
|
| 4 |
A |
313 |
313 |
31.82 |
|
|
|
| 5 |
A |
201 |
201 |
137.67 |
|
|
|
| 6 |
B |
3998 |
3998 |
189.34 |
|
|
|
| 7 |
B |
1529 |
1529 |
388.13 |
|
|
|
| 8 |
B |
571 |
571 |
338.50 |
|
|
|
| 9 |
B |
306 |
306 |
69.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6115.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6115.8 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 B2PLYP=FULL/Def2TZVPP
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
0.006 |
| O2 |
0.000 |
1.429 |
-0.054 |
| O3 |
0.000 |
-1.429 |
-0.054 |
| H4 |
0.555 |
2.042 |
0.416 |
| H5 |
-0.555 |
-2.042 |
0.416 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.4301 | 1.4301 | 2.1556 | 2.1556 |
O2 | 1.4301 | | 2.8576 | 0.9513 | 3.5463 | O3 | 1.4301 | 2.8576 | | 3.5463 | 0.9513 | H4 | 2.1556 | 0.9513 | 3.5463 | | 4.2325 | H5 | 2.1556 | 3.5463 | 0.9513 | 4.2325 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
128.583 |
|
Be1 |
O3 |
H5 |
128.583 |
| O2 |
Be1 |
O3 |
175.226 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability