Jump to
S1C2
Energy calculated at CISD/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -166.210204 |
| Energy at 298.15K | |
| HF Energy | -165.720587 |
| Nuclear repulsion energy | 49.280294 |
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 CISD/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 |
4191 |
3863 |
61.26 |
|
|
|
| 2 |
A1 |
766 |
706 |
4.21 |
|
|
|
| 3 |
A1 |
518 |
477 |
224.31 |
|
|
|
| 4 |
A1 |
286 |
264 |
8.99 |
|
|
|
| 5 |
A2 |
184i |
170i |
0.00 |
|
|
|
| 6 |
B1 |
338 |
311 |
73.91 |
|
|
|
| 7 |
B2 |
4188 |
3860 |
212.08 |
|
|
|
| 8 |
B2 |
1571 |
1449 |
459.80 |
|
|
|
| 9 |
B2 |
417 |
384 |
267.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6044.9 cm
-1
Scaled (by 0.9218) Zero Point Vibrational Energy (zpe) 5572.2 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 CISD/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
-0.006 |
| O2 |
0.000 |
1.415 |
0.071 |
| O3 |
0.000 |
-1.415 |
0.071 |
| H4 |
0.000 |
2.115 |
-0.558 |
| H5 |
0.000 |
-2.115 |
-0.558 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.4174 | 1.4174 | 2.1856 | 2.1856 |
O2 | 1.4174 | | 2.8306 | 0.9409 | 3.5858 | O3 | 1.4174 | 2.8306 | | 3.5858 | 0.9409 | H4 | 2.1856 | 0.9409 | 3.5858 | | 4.2296 | H5 | 2.1856 | 3.5858 | 0.9409 | 4.2296 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
134.894 |
|
Be1 |
O3 |
H5 |
134.894 |
| O2 |
Be1 |
O3 |
173.734 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at CISD/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -166.210765 |
| Energy at 298.15K | -166.212086 |
| HF Energy | -165.721178 |
| Nuclear repulsion energy | 49.255734 |
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 CISD/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 |
4179 |
3852 |
28.50 |
|
|
|
| 2 |
A |
762 |
702 |
1.41 |
|
|
|
| 3 |
A |
508 |
469 |
108.19 |
|
|
|
| 4 |
A |
307 |
283 |
40.62 |
|
|
|
| 5 |
A |
173 |
159 |
155.85 |
|
|
|
| 6 |
B |
4176 |
3849 |
230.96 |
|
|
|
| 7 |
B |
1570 |
1448 |
452.54 |
|
|
|
| 8 |
B |
500 |
461 |
367.81 |
|
|
|
| 9 |
B |
296 |
273 |
75.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6235.4 cm
-1
Scaled (by 0.9218) Zero Point Vibrational Energy (zpe) 5747.8 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 CISD/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
-0.001 |
| O2 |
0.000 |
1.418 |
-0.048 |
| O3 |
0.000 |
-1.418 |
-0.048 |
| H4 |
0.520 |
2.072 |
0.387 |
| H5 |
-0.520 |
-2.072 |
0.387 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.4190 | 1.4190 | 2.1708 | 2.1708 |
O2 | 1.4190 | | 2.8363 | 0.9416 | 3.5552 | O3 | 1.4190 | 2.8363 | | 3.5552 | 0.9416 | H4 | 2.1708 | 0.9416 | 3.5552 | | 4.2719 | H5 | 2.1708 | 3.5552 | 0.9416 | 4.2719 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
132.708 |
|
Be1 |
O3 |
H5 |
132.708 |
| O2 |
Be1 |
O3 |
176.145 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability