-Poisson-Nernst-Planck-Theory-Approach-to-the-calculation-of-ion-泊松能斯特-普朗克理论对离子课件.ppt
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- Poisson Nernst Planck Theory Approach to the calculation of ion 泊松能斯特 普朗克 理论 离子 课件
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1、Poisson-Nernst-Planck Theory Approach to the calculation of ion transport through protein channelsGuozhen ZhangIon transport through protein channels“We human beings consist to about70%of salt water.This years Nobel Prize in Chemistry rewards two scientists whose discoveries have clarified how salts
2、(ions)and water are transported out of and into the cells of the body This is of great importance for our understanding of many diseases of e.g.the kidneys,heart,muscles and nervous system.“(Press release of the Nobel Prize in Chemistry 2019;Doyle,et al.,2019)Theoretical study of ion channels Kineti
3、c models Electrodiffusion models Stochastic models Molecular Dynamics Brownian Dynamics(Kurnikova,et al.,2019;Coalson and Kurnikova,2019)Poisson-Nernst-Planck theory Basic idea Numerical solution Validity Application to Gramicidin A channel Improvement SummaryPreconditions of PNP theory Coarse grain
4、ed approximation mobile ions continuous charge distribution surroundings 3D grid with different dielectric constant High-friction assumption Brownian motion Smoluchowski equation Steady-state assumption the particle flux is time-independent(Kurnikova,et al.,2019)standard PNP theory Nernst-Planck equ
5、ation Poisson equation Total Potential Energy iii0()()();1,.,c Rc RV RiN fii1()()4()()NiRRRqc R ii()()()V RU RqR(Kurnikova,et al.,2019)Solving 3D Poisson equation on a cubic grid 1D case a.division of grid where the lattice cell extends from(j-1/2)h to(j-1/2)h b.discretization of Poisson equation on
6、 the grid 3D case where ij is the 3D generalization of the matrix defined in the above equation,bi(D)are the effective source terms associated with the Dirichlet boundary condition.(Graf,et al.,2000)i,j+1,ki,j-1,ki-1,j,ki+1,j,ki,j,k+1i,j,k-1i,j,kx1ijx1ijy1jjy1jjz1kjz1kjSolving 3D NP Eq.by successive
7、 over-relaxation2/)(2/)(,1,1,1,1x1jijijijijijijijiiccVVccaDDji.Flux x1ijii.Steady-state flux condition001111x1x1zkzkyjyjiijjjjjjjiii.Concentration for central pointeffNiiifeNiiiiDVVDcVVcf10100)(2/(1)(2/(1 Where ,is the number of nearest-neighbor lattice points2/)(0DDDiieffNiv.SOR iteration equation0
8、)1(wccwcoldii1w;(Crdenas,et al.,2000;Kurnikova,et al.,2019)Calibration of the accuracy of the 3D code(Kurnikova,et al.,2019)Application to Gramicidin A channel(Kurnikova,et al.,2019)(Kurnikova,et al.,2019)(Kurnikova,et al.,2019)Comparison with experiments(Kurnikova,et al.,2019)standard PNP theory Ne
9、rnst-Planck equation Poisson equation Total Potential Energy iii0()()();1,.,c Rc RV RiN fii1()()4()()NiRRRqc R ii()()()V RU RqR(Kurnikova,et al.,2019)Dielectric-Energy PNP theory)()()()(0iiiirrcrcrD)()()(iSIPmobileiirGrqriiimobile)(4)()(rcqrr)()()(iDSEproteiniiSIPrGrqrGNernst-Planck equationPoisson
10、equationThe free energy of ions of species i in solution)()(4)()(fiiirrcqrr)()()(iDSEiirGrqri21DSEi2()(,)Grq g r r(Graf,et al.,2019;Coalson and Kurnikova,2019)Performance of DSEPNP(Coalson and Kurnikova,2019)Potential of Mean Force PNP theoryThe protein structure used in both BD and DSEPNP simulatio
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