Title: Electrostatics
1Electrostatics
- Poisson-Boltzmann equation
- finite-difference
- see review by Sharp and Honig (1990)
- Delphi
- GRASP
- solvation energy
- interactions
- Generalized-Born
2Poisson-Boltzmann equation
- Laplace equation
- Poisson equation
- potentials must meet at dielectric boundary
- Poisson-Boltzmann equation
- effect of ions in solvent on potential field
- zi is charge of ion i, ci is concentration
- salt/ionic effects counter-ions move in solvent
to adjust local concentration to local potential
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4for 11 salts, alternative form is
5DELPHI (Honig)
Nicholls and Honig (1991, JCompChem)
Honig and Nicholls (1995, Science)
Jacobian relaxation
6How to use Delphi
- https//www.scripps.edu/rc/softwaredocs/msi/insigh
t2K/delphi/delphiTOC.html - http//bcr.musc.edu/manuals/delphi.htm
- param files (copy to local directory)
- parseres.siz, parseres.crg (Sitkoff, Sharp,
Honig, 1994) polar Hs, vdw radii, and partial
charges for aas and nas) note
HIS/HID/HIE/HIP - check hydrogen names
- script
- unixgt delphi lt delphi.in gt delphi.out
- output
- energies in log file
- check net assigned charge
- ltpotential_mapgt.phi (for GRASP or chimera)
- potentials at specific coords
dhfr.in ------- gsize65 scale1.0 in(pdb,file"dh
fr.pdb") in(siz,file"parseres.siz") in(crg,file"
parseres.crg") indi4.0 exdi80.0 prbrad1.4 salt
0.10 bndcon2 maxc0.0001 !linit800 nonit800 ene
rgy(s,c,g) out(phi,file"dhfr-mesh.phi") in(frc,fi
le"dhfr-mesh.pdb") out(frc,file"dhfr-mesh.pot")
site(a,x,p,q)
1 kT 0.592 kcal/mol for T 298 K and k
0.001986577 kcal/molK
(1) total grid energy 5168.769
kt (2) self-reaction field energy
-19088.44 kt (3) total s.charge,no epsin
carrying 1.4302 (4) corrected reaction field
energy -782.8139 kt (5) total reaction
field energy -19871.26 kt (6) coulombic
energy -8125.605 kt (7) All
energy terms but grid and self_react. -8908.419
kt
1 kT 0.592 kcal/mol for T 298 K and k
0.001986577 kcal/molK
7Uses of Delphi
- Calculation of pKas
- place a test charge, evaluate potential, dont
forget to subtract solvation energy of test
charge - Calculation of binding energies (P-P complexes)
- Do 3 runs A (apo/solvated), B (apo/solv), AB
(complex) - reviews
- Gilson and Honig (1988)
- Sheinerman, Norel, Honig (2000)
- Sheinerman and Honig (2002, JMB)
- study of 4 complexes barnasebarstar, human
growth hormone receptror, neuraminidaseantibody,
Raskinase - role of polar vs. non-polar interactions varies
(show correlation plot of binding affinities
with estimates via delphi)
8- examples of Delphi potentials mapped onto
molecular surfaces (using GRASP)
acetylcholine esterase
DNA-binding proteins from DNA polymerase
III subunit b
9Solvation Energy
- important for interactions
- free energy of binding involves desolvation of
receptor and ligand (polar and non-polar
contributions) - total electrostatic energy of molecule includes
- Coulombic interaction of charges (and dipoles),
- plus energy due to solvent reaction field
(charges attracted to surface) - self energy int. charge with induced surface
charges - cross terms reduction in charge-charge
interactions by attracted surface charges to
other (solvent screening) - Gilson and Honig (1988)
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11reaction field energy
- in Delphi, total energy includes grid energy,
must subtract out - do calculations twice
- once for vacuum (e1) and once for water (e80)
- take difference of potentials at each grid point
- alternatively calculate charges at surface
positions - mapping to fixed grid creates approximation error
- can scale surface points to molecular surface
to increase accuracy - these are the corrected reaction field energies
in Delphi
di are surface charges qj are molecule charges
12Non-polar term, DGsolv,np
- cavity formation VDW attraction
- weak, typically proportional to surface area (SA)
- Sitkoff Sharp Honig (1994)
- fit for alkanes
- g5.0 0.5 cal/mol Å2
- b0.86 0.1 kcal/mol
- depends on curvature of cavity
- Massova Kollman (2000), Ferrari et al (2007)
use g7.2 cal/mol Å2 (b0) or g5.4 cal/mol Å2
(b0.92 kcal/mol) - gcav-38, gvdw46 (Noskov Friedman)
- Levy et al (JACS, 2003) On the Non-polar
Hydration Free Energy...
http//dx.doi.org/10.1016/j.bmc.2007.08.019 see
footnote to Table 1
13Interactions
- difference of energy of apo vs. complex in
solvent vs. vacuum
- over half of complex have substantial changes
between - apo and complexed forms (Betts Sternberg,
1999) - energy related to induced fit (Noskov and Lim,
2001) - Marilyn Gunner
14Implicit Models of Solvation
- avoid solving PBE for potential too slow for
dynamics/docking - model DGsol via scaling of charge-charge
interactions according to depth of buriedness - depends on solvent-accessible surface, shape of
dielectric boundary
15Generalized Born Approximation
- The goal of GB theory can be thought of as an
effort to find a relatively simple analytical
formula, resembling Equation 6, which for real
molecular geometries will capture, as much as
possible, the physics of the Poisson equation. - Born approximation for ion (point charge in
sphere of atomic radius) - use effective Born radii Ri,Rj to scale
charge-charge interactions
(eqn. 6)
(1/f for RiRj1/2)
16from Warshel, Russel, Churg (1984)
17Effective Born radius
(show increase in effective Born radius with
depth of burial...)
calculation requires integration over volume of
the molecule (shape)
18Methods to calculate Born radii
- replace volume integration (1/r4) with
atom-pairwise computation - methods
- Still et al (1990) numeric integration
- Qui (1997) add volumes of atoms
- Ghosh Rapp Friesner (1998) surface integral
- Hawkins Cramer Truhlar (1996)
- analytic formula for 1/r4 in sphere
- radii scaling params to account for overlaps
- Liu Kuntz Zou (2004) grid in DOCK
- Dominy Brooks (1999) re-fit params for CHARMM
bend 1-3 connected atoms stretch 1-2 connected
atoms CCF close-contact function
19- GB-solv can be added as term in AMBER FF
- calculation of solvation params (effective Born
radii) - changes with shape/conformation
- see AMBER 10 manual
- also SASA term in CHARMM 19 (EFF1)
- Warshel, Russell, Churg (1984) self-energy
- Onsager energy of buried dipole