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All results from a given calculation for Be(OH)2 (Beryllium hydroxide)

using model chemistry: CCD/6-311+G(3df,2p)

19 10 17 12 22

States and conformations

State Conformation minimum conformation conformer description state description
1 1 no C2V 1A1
1 2 yes C2 1A

Conformer 1 (C2V)

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 energy49.084355
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
4/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.
Rotational Constants (cm-1) from geometry optimized at CCD/6-311+G(3df,2p)
ABC
21.47936 0.22910 0.22669

See section I.F.4 to change rotational constant units
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
Be11.42271.42272.19102.1910
O21.42272.84030.94653.5975
O31.42272.84033.59750.9465
H42.19100.94653.59754.2413
H52.19103.59750.94654.2413

picture of Beryllium hydroxide state 1 conformation 1
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

Conformer 2 (C2)

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 energy49.048568
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
4/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.
Rotational Constants (cm-1) from geometry optimized at CCD/6-311+G(3df,2p)
ABC
19.17087 0.22795 0.22762

See section I.F.4 to change rotational constant units
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
Be11.42481.42482.17322.1732
O21.42482.84780.94733.5626
O31.42482.84783.56260.9473
H42.17320.94733.56264.2736
H52.17323.56260.94734.2736

picture of Beryllium hydroxide state 1 conformation 2
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