An electrostatic model for the dielectric effects, the adsorption of multivalent ions, and the bending of B-DNA

✍ Scribed by Dirk Stigter

• Publisher: Wiley (John Wiley & Sons)
• Year: 1998
• Tongue: English
• Weight: 202 KB
• Volume: 46
• Category: Article
• ISSN: 0006-3525
• DOI: 10.1002/(sici)1097-0282(199812)46:7<503::aid-bip8>3.0.co;2-v

✦ Synopsis

We have studied electrostatic properties of DNA with a discrete charge model consisting of a cylindrical dielectric core with a radius of 8 Å and a dielectric constant D i ϭ 4, surrounded by two helical strings of phosphate point charges at 10 Å from the axis, immersed in an aqueous medium with dielectric constant D w ϭ 78.54. Eliminating the dielectric core makes potentials in the phosphate surface less negative by about 0.5 kT/e. Salt effects are evaluated for the model without a dielectric core, using the shielded Coulomb potential. Smearing the phosphate charges increases their potential by about 2.5 kT/e, due mostly to the self-potential of the smeared charge. Potentials in the center of the minor and major grooves vary less than 0.02 kT/e along their helical path. The potential in the center of the minor groove is from 1.0 to 1.7 kT/e, more negative than in the center of the major groove, depending on dielectric core and salt concentration. So multivalent cations and also larger cationic ligands, such as some antibiotics, are likely to adsorb in the minor groove, in agreement with earlier computations by A. and B. Pullman. Dielectric effects on the surface potential and the local potential variations are found to be relatively small. Bending of DNA is studied by placing a multivalent cation, M Zϩ , in the center of the minor or major groove, curving DNA around it for a certain length, and calculating the free energy difference between the bent and the straight configuration. Boltzmann averaged bending angles, ͗␤͘, are found to be maximal in 0.03M monovalent salt, for a length of about 50 or 25 Å of curved DNA when an M Zϩ ion is adsorbed in the minor or the major groove, respectively. When the dielectric constant of water is used throughout the calculation, we find maximal bends of ͗␤͘ ϭ 11°for M 2ϩ and ͗␤͘ ϭ 16°for M 3ϩ in the minor groove, ͗␤͘ ϭ 13°for M 3ϩ in the major groove. The absence of bends in DNA adsorbed to mica in the presence of Mg salts supports the role of Mg 2ϩ in "ion bridging" between DNA and mica. The treatment of the effective dielectric constant between two points outside a dielectric cylinder in water is appended.