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

using model chemistry: CCSD(T)=FULL/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 CCSD(T)=FULL/6-311+G(3df,2p)
 hartrees
Energy at 0K-166.345666
Energy at 298.15K 
HF Energy-165.720007
Nuclear repulsion energy49.136247
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 CCSD(T)=FULL/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 4060 4060        
2 A1 753 753        
3 A1 476 476        
4 A1 281 281        
5 A2 186i 186i        
6 B1 326 326        
7 B2 4059 4059        
8 B2 1538 1538        
9 B2 371 371        

Unscaled Zero Point Vibrational Energy (zpe) 5838.9 cm-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5838.9 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.
Rotational Constants (cm-1) from geometry optimized at CCSD(T)=FULL/6-311+G(3df,2p)
ABC
22.53075 0.22977 0.22745

See section I.F.4 to change rotational constant units
Geometric Data calculated at CCSD(T)=FULL/6-311+G(3df,2p)

Point Group is C2v

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
Be1 0.000 0.000 -0.026
O2 0.000 1.416 0.074
O3 0.000 -1.416 0.074
H4 0.000 2.137 -0.542
H5 0.000 -2.137 -0.542

Atom - Atom Distances (Å)
  Be1 O2 O3 H4 H5
Be11.41971.41972.19872.1987
O21.41972.83240.94843.6066
O31.41972.83243.60660.9484
H42.19870.94843.60664.2747
H52.19873.60660.94844.2747

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 135.456 Be1 O3 H5 135.456
O2 Be1 O3 171.917
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability

Conformer 2 (C2)

Jump to S1C1
Energy calculated at CCSD(T)=FULL/6-311+G(3df,2p)
 hartrees
Energy at 0K-166.346205
Energy at 298.15K-166.347408
HF Energy-165.720632
Nuclear repulsion energy49.091987
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 CCSD(T)=FULL/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 4045 4045        
2 A 747 747        
3 A 462 462        
4 A 294 294        
5 A 173 173        
6 B 4043 4043        
7 B 1534 1534        
8 B 453 453        
9 B 280 280        

Unscaled Zero Point Vibrational Energy (zpe) 6014.6 cm-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6014.6 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 CCSD(T)=FULL/6-311+G(3df,2p)
ABC
19.89239 0.22856 0.22825

See section I.F.4 to change rotational constant units
Geometric Data calculated at CCSD(T)=FULL/6-311+G(3df,2p)

Point Group is C2

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
Be1 0.000 0.000 0.013
O2 0.000 1.420 -0.052
O3 0.000 -1.420 -0.052
H4 0.517 2.086 0.386
H5 -0.517 -2.086 0.386

Atom - Atom Distances (Å)
  Be1 O2 O3 H4 H5
Be11.42201.42202.18102.1810
O21.42202.84100.94943.5711
O31.42202.84103.57110.9494
H42.18100.94943.57114.2978
H52.18103.57110.94944.2978

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 132.776 Be1 O3 H5 132.776
O2 Be1 O3 174.792
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability