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:
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Computer Science and Genome Center
The electric flux out of any closed surface is proportional to the
total charge enclosed within the surface.
- 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
(charge density = 0)
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)
a shell of positive
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
Modified Poisson equation:
Energies are scaled by the same factor. For two charges:
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…)
This equation is difficult to solve for a system like a macromolecule!!
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!
I: ionic strength
j : indices of the six direct neighbors of i
Solve as a large system of linear
An example of the self-intersection of molecular surface
Comparison between the molecular surface model and the skin model for a protein
card(X) =1, 4
card(X) =2, 3
Join the points to form a mesh of triangles
A 2D illustration of skin surface meshing algorithm
Full Delaunay of sampling points
Restricted Delaunay defining
the skin surface mesh
Triangle quality distribution
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