z-logo
Premium
Ligand‐Exchange Processes on Solvated Beryllium Cations. Part III
Author(s) -
Puchta Ralph,
van Eldik Rudi
Publication year - 2008
Publication title -
helvetica chimica acta
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.74
H-Index - 82
eISSN - 1522-2675
pISSN - 0018-019X
DOI - 10.1002/hlca.200890114
Subject(s) - chemistry , ligand (biochemistry) , activation barrier , activation energy , crystallography , molecule , cluster (spacecraft) , beryllium , solvent , density functional theory , computational chemistry , biochemistry , receptor , organic chemistry , computer science , programming language
Abstract On the basis of DFT calculations (B3LYP/6‐311+G**), the possibility to include solvent effects is considered in the investigation of the H 2 O‐exchange mechanism on [Be(H 2 O) 4 ] 2+ within the widely used cluster approach. The smallest system in the gas phase, [Be(H 2 O) 4 (H 2 O)] 2+ , shows the highest activation barrier of +15.6 kcal/mol, whereas the explicit addition of five H‐bonded H 2 O molecules in [{Be(H 2 O) 4 (H 2 O)}(H 2 O) 5 ] 2+ reduces the barrier to +13.5 kcal/mol. Single‐point calculations applying CPCM (B3LYP(CPCM:H 2 O)/6‐311+G**//B3LYP/6‐311+G**) on [Be(H 2 O) 4 (H 2 O)] 2+ lower the barrier to +9.6 kcal/mol. Optimization of the precursor and transition state of [Be(H 2 O) 4 (H 2 O)] 2+ within an implicit model (B3LYP(CPCM:H 2 O)/6‐311+G** or B3LYP(PCM:H 2 O)/6‐311+G**) reduces the activation energy further to +8.3 kcal/mol but does not lead to any local minimum for the precursor and is, therefore, unfavorable.

This content is not available in your region!

Continue researching here.

Having issues? You can contact us here