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Poisson-Nernst-Planck Theory Approach to the calculation of ion transport through protein channels

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Title: Poisson-Nernst-Planck Theory Approach to the calculation of ion transport through protein channels


1
Poisson-Nernst-Planck Theory Approach to the
calculation of ion transport through protein
channels
  • Guozhen Zhang

2
Ion transport through protein channels
  • We human beings consist to about
  • 70 of salt water. This year's Nobel
  • Prize in Chemistry rewards two
  • scientists whose discoveries have
  • clarified how salts (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
2003 Doyle, et al., 1998)
3
Theoretical study of ion channels
  • Kinetic models
  • Electrodiffusion models
  • Stochastic models
  • Molecular Dynamics
  • Brownian Dynamics

(Kurnikova, et al., 1999 Coalson and Kurnikova,
2005)
4
Poisson-Nernst-Planck theory
  • Basic idea
  • Numerical solution
  • Validity
  • Application to Gramicidin A channel
  • Improvement
  • Summary

5
Preconditions of PNP theory
  • Coarse grained approximation
  • mobile ions gt continuous charge distribution
  • surroundings gt 3D grid with different
    dielectric constant
  • High-friction assumption
  • Brownian motion gt Smoluchowski equation
  • Steady-state assumption
  • the particle flux is time-independent

(Kurnikova, et al., 1999)
6
standard PNP theory
  • Nernst-Planck equation
  • Poisson equation
  • Total Potential Energy

(Kurnikova, et al., 1999)
7
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 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)
8
Solving 3D NP Eq. by successive over-relaxation
i. Flux
ii. Steady-state flux condition
iii. Concentration for central point
Where ,
is the number of nearest-neighbor lattice points
(Cárdenas, et al., 2000 Kurnikova, et al., 1999)
iv. SOR iteration equation
9
Calibration of the accuracy of the 3D code
(Kurnikova, et al., 1999)
10
Application to Gramicidin A channel
(Kurnikova, et al., 1999)
11
(Kurnikova, et al., 1999)
12
(Kurnikova, et al., 1999)
13
Comparison with experiments
(Kurnikova, et al., 1999)
14
standard PNP theory
  • Nernst-Planck equation
  • Poisson equation
  • Total Potential Energy

(Kurnikova, et al., 1999)
15
Dielectric-Energy PNP theory
Nernst-Planck equation
Poisson equation
The free energy of ions of species i in solution
(Graf, et al., 2004 Coalson and Kurnikova, 2005)
16
Performance of DSEPNP
(Coalson and Kurnikova, 2005)
17
Potential of Mean Force PNP theory
  • The protein structure used in both BD and DSEPNP
    simulations is taken to be rigid, while in
    reality the protein structure responds
    dynamically to an ions presence. Such a defect
    usually exhibits very small superlinear currents
    for voltages up to 200mV for narrow channels.
  • This issue can in principle be solved by a full
    atomistic simulation which requires complete
    sampling of the system configuration space. But
    its formidable for current computing capability.
  • Limited sampling of the environment
    configurational space has been introduced to deal
    with the problem. A combined MD/continuum
    electrostatics approach is then proposed to
    obtain ?GSIP at an average solvent effect level,
    which is then used in PNP formalism. Such a
    procedure is termed PMFPNP.

(Coalson and Kurnikova, 2005)
18
Results of the PMFPNP calculations
  • The overall structure of peptide doesnt change
    much over the course of MD trajectory, so the
    ?GDSE contribution to the overall ?GSIP doesnt
    vary much.
  • Small local distortions of pore-lining parts of
    the peptide (especially carbonyl groups)
    significantly stabilize cations as they move
    through it.
  • PMFPNP theory is able to account for effects that
    are beyond the reach of primitive PNP theory,
    namely, saturation of ion current through the
    channel as the concentration of bathing solutions
    increases to a sufficiently high value.

(Coalson and Kurnikova, 2005)
19
The saturation mechanism
(Coalson and Kurnikova, 2005)
20
Summary
  • 3D PNP theory is of conceptual simplicity. It
    relies on a caricature of the microscopic world
    in which background media are treated as
    dielectric slabs and the mobile ions of interest
    are smeared out into a continuous charge
    distribution.
  • The inherent restriction of the theory is mainly
    due to its simplicity. It may be unrealistic for
    treating certain properties of certain ion
    channels. Also, the mean-field continuum
    solvent/ion theory of this type is inadequate to
    accurately describe the underlying dynamics.
  • Despite of these restrictions, PNP theory will
    continue to play a useful role in computing and
    understanding the kinetics of ion permeation
    through (wider) biological channels.

(Coalson and Kurnikova, 2005)
21
References
  • Cárdenas, A. E., R. D. Coalson, and M. G.
    Kurnikova. 2000. Three-Dimensional
    Poisson-Nernst-Planck Theory Studies Influence
    of Membrane Electrostatics on Gramicidin A
    Channel Conductance. Biophys. J. 79 80-93.
  • Coalson, R. D., and M. G. Kurnikova. 2005.
    PoissonNernstPlanck Theory Approach to the
    Calculation of Current Through Biological Ion
    Channels. IEEE T Nanobiosci. 4 81-93.
  • Doyle, D.A., J. M. Cabral, R. A. Pfuetzner, A.
    Kuo, J. M. Gulbis, S. L. Cohen, B.T. Chait, and
    R. MacKinnon. 1998. The structure of the
    potassium channel Molecular basis of
    K conduction and selectivity. Science. 280
    69-77.
  • Graf, P., A. Nitzan, M. G. Kurnikova, and R. D.
    Coalson. 2000. A dynamic lattice Monte Carlo
    model of ion transport in inhomogeneous
    dielectric environments Method and
    implementation. J. Phys. Chem. B. 104
    12324-12338.
  • Graf, P., M. Kurnikova, R. Coalson, and A.
    Nitzan. 2004. Comparison of dynamic lattice Monte
    Carlo simulations and the dielectric self-energy
    Poisson-Nernst-Planck continuum theory for model
    ion channels. J. Phys. Chem. B. 108 2006-2015.
  • Kurnikova, M. G., R. D. Coalson, P. Graf, and A.
    Nitzan. 1999. A lattice relaxation algorithm for
    three-dimensional Poisson-Nernst-Planck theory
    with application to ion transport through the
    gramicidinA channel. Biophys. J. 76 642656.

22
Thank you!
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