Electrical potential of transfer RNAs: codon-anticodon recognition

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Abstract
Calculations of the electrostatic potentials were made around yeast elongator phenylalanine, aspartate tRNAs, and yeast initiator methionine tRNA in aqueous solution at physiological ionic strength. The calculations were carried out with a finite difference algorithm for solving the nonlinear Poisson-Boltzmann, equation that incorporates the screening effects of the electrolyte, the exclusion of ions by the molecule, the molecular shape, and the different polarizabilities of the solvent and the tRNA. The initiator tRNA is surrounded by uniformly spaced contours of negative potential. The elongator tRNA are also surrounded by a similar contour pattern except in the anticodon region where there is a pronounced "hole" in the potential surface. This hole is caused by an invagination of the potential contours, which also results in an increase in the local field strength. The effect of this hole is that the anticodon region in the elongator tRNAs is the least negative, or conversely the most positive, region of the molecule. This hole, which is not found when simple Coulombic potentials are used, is due both to the structure of the elongator tRNA anticodon loops and to the different polarizabilities of the solvent and tRNA. The existence of the potential hole in elongator tRNAs may account in part for their ability to associate with other negatively charged macromolecules, in particular mRNA. Moreover, it suggests that the anticodon loop of elongator tRNAs is the energetically most favorable point of approach of mRNA to tRNA.