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

using model chemistry: B2PLYP=FULL/cc-pVDZ

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 B2PLYP=FULL/cc-pVDZ
 hartrees
Energy at 0K-166.378812
Energy at 298.15K 
HF Energy-166.239030
Nuclear repulsion energy48.602769
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/cc-pVDZ
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 3964 3799 68.05      
2 A1 738 708 13.45      
3 A1 621 595 121.67      
4 A1 295 283 13.12      
5 A2 211i 202i 0.00      
6 B1 337 323 63.49      
7 B2 3961 3797 139.14      
8 B2 1536 1472 291.68      
9 B2 500 480 290.16      

Unscaled Zero Point Vibrational Energy (zpe) 5870.7 cm-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 5627.1 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 B2PLYP=FULL/cc-pVDZ
ABC
15.61268 0.22612 0.22289

See section I.F.4 to change rotational constant units
Geometric Data calculated at B2PLYP=FULL/cc-pVDZ

Point Group is C2v

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
Be1 0.000 0.000 0.017
O2 0.000 1.439 0.080
O3 0.000 -1.439 0.080
H4 0.000 2.031 -0.674
H5 0.000 -2.031 -0.674

Atom - Atom Distances (Å)
  Be1 O2 O3 H4 H5
Be11.44041.44042.14522.1452
O21.44042.87790.95853.5510
O31.44042.87793.55100.9585
H42.14520.95853.55104.0622
H52.14523.55100.95854.0622

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 125.625 Be1 O3 H5 125.625
O2 Be1 O3 174.940
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability

Conformer 2 (C2)

Jump to S1C1
Energy calculated at B2PLYP=FULL/cc-pVDZ
 hartrees
Energy at 0K-166.379506
Energy at 298.15K-166.381044
HF Energy-166.239506
Nuclear repulsion energy48.571076
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/cc-pVDZ
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 3942 3779 45.04      
2 A 733 702 7.48      
3 A 620 595 77.02      
4 A 299 286 13.09      
5 A 244 234 104.10      
6 B 3941 3777 147.69      
7 B 1532 1469 285.62      
8 B 592 567 309.24      
9 B 297 285 85.68      

Unscaled Zero Point Vibrational Energy (zpe) 6099.8 cm-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 5846.7 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 B2PLYP=FULL/cc-pVDZ
ABC
14.29863 0.22491 0.22416

See section I.F.4 to change rotational constant units
Geometric Data calculated at B2PLYP=FULL/cc-pVDZ

Point Group is C2

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
Be1 0.000 0.000 -0.034
O2 0.000 1.442 -0.061
O3 0.000 -1.442 -0.061
H4 0.508 1.978 0.553
H5 -0.508 -1.978 0.553

Atom - Atom Distances (Å)
  Be1 O2 O3 H4 H5
Be11.44261.44262.12482.1248
O21.44262.88460.95993.5119
O31.44262.88463.51190.9599
H42.12480.95993.51194.0843
H52.12483.51190.95994.0843

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 123.096 Be1 O3 H5 123.096
O2 Be1 O3 177.855
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability