1 / 27

The Geometry of Biomolecular Solvation 2. Electrostatics

The Geometry of Biomolecular Solvation 2. Electrostatics. Patrice Koehl Computer Science and Genome Center http://www.cs.ucdavis.edu/~koehl/. Solvation Free Energy. W sol. +. +. W np. A Poisson-Boltzmann view of Electrostatics. Elementary Electrostatics in vacuo. Gauss’s law:

bliss
Download Presentation

The Geometry of Biomolecular Solvation 2. Electrostatics

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. The Geometry of Biomolecular Solvation2. Electrostatics Patrice Koehl Computer Science and Genome Center http://www.cs.ucdavis.edu/~koehl/

  2. Solvation Free Energy Wsol + + Wnp

  3. A Poisson-Boltzmann view of Electrostatics

  4. Elementary Electrostatics in vacuo Gauss’s law: The electric flux out of any closed surface is proportional to the total charge enclosed within the surface. Integral form: Differential form: Notes: - for a point charge q at position X0, r(X)=qd(X-X0) - Coulomb’s law for a charge can be retrieved from Gauss’s law

  5. Elementary Electrostatics in vacuo Poisson equation: Laplace equation: (charge density = 0)

  6. Uniform Dielectric Medium Physical basis of dielectric screening An atom or molecule in an externally imposed electric field develops a non zero net dipole moment: - + (The magnitude of a dipole is a measure of charge separation) The field generated by these induced dipoles runs against the inducing field the overall field is weakened (Screening effect) The negative charge is screened by a shell of positive charges.

  7. Uniform Dielectric Medium Polarization: The dipole moment per unit volume is a vector field known as the polarization vector P(X). In many materials: c is the electric susceptibility, and e is the electric permittivity, or dielectric constant The field from a uniform dipole density is -4pP, therefore the total field is

  8. Uniform Dielectric Medium Modified Poisson equation: Energies are scaled by the same factor. For two charges:

  9. System with dielectric boundaries The dielectric is no more uniform: e varies, the Poisson equation becomes: If we can solve this equation, we have the potential, from which we can derive most electrostatics properties of the system (Electric field, energy, free energy…) BUT This equation is difficult to solve for a system like a macromolecule!!

  10. The Poisson Boltzmann Equation r(X) is the density of charges. For a biological system, it includes the charges of the “solute” (biomolecules), and the charges of free ions in the solvent: The ions distribute themselves in the solvent according to the electrostatic potential (Debye-Huckel theory): The potential  is itself influenced by the redistribution of ion charges, so the potential and concentrations must be solved for self consistency!

  11. The Poisson Boltzmann Equation Linearized form: I: ionic strength

  12. Solving the Poisson Boltzmann Equation • Analytical solution • Only available for a few special simplification of the molecular shape and charge distribution • Numerical Solution • Mesh generation -- Decompose the physical domain to small elements; • Approximate the solution with the potential value at the sampled mesh vertices -- Solve a linear system formed by numerical methods like finite difference and finite element method • Mesh size and quality determine the speed and accuracy of the approximation

  13. Linear Poisson Boltzmann equation: Numerical solution • Space discretized into a • cubic lattice. • Charges and potentials are • defined on grid points. • Dielectric defined on grid lines • Condition at each grid point: ew eP j : indices of the six direct neighbors of i Solve as a large system of linear equations

  14. Meshes • Unstructured mesh have advantages over structured mesh on boundary conformity and adaptivity • Smooth surface models for molecules are necessary for unstructured mesh generation

  15. Molecular Surface Disadvantages • Lack of smoothness • Cannot be meshed with good quality An example of the self-intersection of molecular surface

  16. Molecular Skin • The molecular skin is similar to the molecular surface but uses hyperboloids blend between the spheres representing the atoms • It is a smooth surface, free of intersection Comparison between the molecular surface model and the skin model for a protein

  17. Molecular Skin • The molecular skin surface is the boundary of the union of an infinite family of balls

  18. Skin Decomposition Hyperboloid patches Sphere patches card(X) =1, 4 card(X) =2, 3

  19. Building a skin mesh Join the points to form a mesh of triangles Sample points

  20. Building a skin mesh A 2D illustration of skin surface meshing algorithm

  21. Building a skin mesh Full Delaunay of sampling points Restricted Delaunay defining the skin surface mesh

  22. Mesh Quality

  23. Mesh Quality Triangle quality distribution

  24. Example Skin mesh Volumetric mesh

  25. Problems with Poisson Boltzmann • Dimensionless ions • No interactions between ions • Uniform solvent concentration • Polarization is a linear response to E, with constant proportion • No interactions between solvent and ions

  26. Modified Poisson Boltzmann Equations Generalized Gauss Equation: Classically, P is set proportional to E. A better model is to assume a density of dipoles, with constant module po Also assume that both ions and dipoles have a fixed size a

  27. Generalized Poisson-Boltzmann Langevin Equation with and

More Related