TY - JOUR
T1 - The ionic atmosphere around A-RNA
T2 - Poisson-Boltzmann and molecular dynamics simulations
AU - Kirmizialtin, Serdal
AU - Silalahi, Alexander R.J.
AU - Elber, Ron
AU - Fenley, Marcia O.
N1 - Funding Information:
This research was supported by National Institutes of Health grant No. GM085062 to R.E. and National Institutes of Health grant No. 5R44GM073391 (Principal Investigator: Dr. Alexander H. Boschitsch) to M.O.F.
PY - 2012/2/22
Y1 - 2012/2/22
N2 - The distributions of different cations around A-RNA are computed by Poisson-Boltzmann (PB) equation and replica exchange molecular dynamics (MD). Both the nonlinear PB and size-modified PB theories are considered. The number of ions bound to A-RNA, which can be measured experimentally, is well reproduced in all methods. On the other hand, the radial ion distribution profiles show differences between MD and PB. We showed that PB results are sensitive to ion size and functional form of the solvent dielectric region but not the solvent dielectric boundary definition. Size-modified PB agrees with replica exchange molecular dynamics much better than nonlinear PB when the ion sizes are chosen from atomistic simulations. The distribution of ions 14 away from the RNA central axis are reasonably well reproduced by size-modified PB for all ion types with a uniform solvent dielectric model and a sharp dielectric boundary between solvent and RNA. However, this model does not agree with MD for shorter distances from the A-RNA. A distance-dependent solvent dielectric function proposed by another research group improves the agreement for sodium and strontium ions, even for shorter distances from the A-RNA. However, Mg 2+ distributions are still at significant variances for shorter distances.
AB - The distributions of different cations around A-RNA are computed by Poisson-Boltzmann (PB) equation and replica exchange molecular dynamics (MD). Both the nonlinear PB and size-modified PB theories are considered. The number of ions bound to A-RNA, which can be measured experimentally, is well reproduced in all methods. On the other hand, the radial ion distribution profiles show differences between MD and PB. We showed that PB results are sensitive to ion size and functional form of the solvent dielectric region but not the solvent dielectric boundary definition. Size-modified PB agrees with replica exchange molecular dynamics much better than nonlinear PB when the ion sizes are chosen from atomistic simulations. The distribution of ions 14 away from the RNA central axis are reasonably well reproduced by size-modified PB for all ion types with a uniform solvent dielectric model and a sharp dielectric boundary between solvent and RNA. However, this model does not agree with MD for shorter distances from the A-RNA. A distance-dependent solvent dielectric function proposed by another research group improves the agreement for sodium and strontium ions, even for shorter distances from the A-RNA. However, Mg 2+ distributions are still at significant variances for shorter distances.
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U2 - 10.1016/j.bpj.2011.12.055
DO - 10.1016/j.bpj.2011.12.055
M3 - Article
C2 - 22385854
AN - SCOPUS:84857256519
SN - 0006-3495
VL - 102
SP - 829
EP - 838
JO - Biophysical journal
JF - Biophysical journal
IS - 4
ER -