Jump to
S1C2
Energy calculated at CCD/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -166.256392 |
| Energy at 298.15K | |
| HF Energy | -165.720169 |
| Nuclear repulsion energy | 49.084355 |
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 CCD/6-311+G(3df,2p)
| 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 |
4102 |
3869 |
53.00 |
|
|
|
| 2 |
A1 |
756 |
713 |
3.93 |
|
|
|
| 3 |
A1 |
514 |
485 |
213.12 |
|
|
|
| 4 |
A1 |
285 |
269 |
8.07 |
|
|
|
| 5 |
A2 |
189i |
179i |
0.00 |
|
|
|
| 6 |
B1 |
334 |
315 |
63.35 |
|
|
|
| 7 |
B2 |
4101 |
3867 |
195.37 |
|
|
|
| 8 |
B2 |
1551 |
1462 |
447.51 |
|
|
|
| 9 |
B2 |
412 |
388 |
266.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5932.2 cm
-1
Scaled (by 0.9431) Zero Point Vibrational Energy (zpe) 5594.7 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 CCD/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
-0.012 |
| O2 |
0.000 |
1.420 |
0.073 |
| O3 |
0.000 |
-1.420 |
0.073 |
| H4 |
0.000 |
2.121 |
-0.563 |
| H5 |
0.000 |
-2.121 |
-0.563 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.4227 | 1.4227 | 2.1910 | 2.1910 |
O2 | 1.4227 | | 2.8403 | 0.9465 | 3.5975 | O3 | 1.4227 | 2.8403 | | 3.5975 | 0.9465 | H4 | 2.1910 | 0.9465 | 3.5975 | | 4.2413 | H5 | 2.1910 | 3.5975 | 0.9465 | 4.2413 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
134.279 |
|
Be1 |
O3 |
H5 |
134.279 |
| O2 |
Be1 |
O3 |
173.082 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at CCD/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -166.256978 |
| Energy at 298.15K | -166.258280 |
| HF Energy | -165.720768 |
| Nuclear repulsion energy | 49.048568 |
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 CCD/6-311+G(3df,2p)
| 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 |
4090 |
3858 |
25.44 |
|
|
|
| 2 |
A |
751 |
708 |
1.42 |
|
|
|
| 3 |
A |
507 |
478 |
102.11 |
|
|
|
| 4 |
A |
302 |
285 |
35.24 |
|
|
|
| 5 |
A |
171 |
162 |
149.84 |
|
|
|
| 6 |
B |
4089 |
3856 |
207.17 |
|
|
|
| 7 |
B |
1548 |
1460 |
438.13 |
|
|
|
| 8 |
B |
498 |
470 |
355.82 |
|
|
|
| 9 |
B |
292 |
275 |
73.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6124.1 cm
-1
Scaled (by 0.9431) Zero Point Vibrational Energy (zpe) 5775.6 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 CCD/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
0.002 |
| O2 |
0.000 |
1.424 |
-0.050 |
| O3 |
0.000 |
-1.424 |
-0.050 |
| H4 |
0.527 |
2.071 |
0.398 |
| H5 |
-0.527 |
-2.071 |
0.398 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.4248 | 1.4248 | 2.1732 | 2.1732 |
O2 | 1.4248 | | 2.8478 | 0.9473 | 3.5626 | O3 | 1.4248 | 2.8478 | | 3.5626 | 0.9473 | H4 | 2.1732 | 0.9473 | 3.5626 | | 4.2736 | H5 | 2.1732 | 3.5626 | 0.9473 | 4.2736 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
131.694 |
|
Be1 |
O3 |
H5 |
131.694 |
| O2 |
Be1 |
O3 |
175.785 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability