Re: [Apbs-users] Electrostatic Free energy of folding in water (per residue)
Biomolecular electrostatics software
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From: Nathan B. <nat...@ma...> - 2006-10-05 11:00:22
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Hi Steve -- > I am still missing something. > Lets see if this diagram helps: > > Folded State in water (Faq) > Unfolded State in water (Uaq) - residue from the pqr file without =20 > changing its position > Folded State Vacuum (Fv) > Unfolded State Vacuum (Uv) > > DG,elec,v > Uv <--> Fv > DGu,solv | | || DGf,solv > Uaq <--> Faq > DG,elec,aq > > DGf,solv =3D Faq-Fv (where values for each state are from APBS) > DG,elec,v =3D Fv-Uv > DGu,solv =3D Uaq-Uv This seems reasonable. > I think DG,elec,aq should be on the order of ~1kcal/(mol res). > Calculating directly gives values that are approximately 100 times =20 > too large in magnitude. > =46rom your e-mail, I think you are saying: > > DG,elec,v+DGf,solv-DGu,solv Yes, this is how I would calculate it. > But this gives the same value because the vacuum terms cancel. > (i.e. Fv-Uv+Faq-Fv-Uaq+Uv=3DFaq-Uaq) Be careful about this cancellation. Coulombic interactions aren't =20 reproduced accurately by PB solvers due to grid artifacts and the =20 inclusion of self interactions. Removal of these self-interactions =20 through the free energy cycle I mentioned is *almost always* =20 necessary for accurate answers. The symptom of failing to remove =20 these interactions are very large energies. > It seems I am misunderstanding something obvious, but I don=92t know =20= > what. > > Oddly, > DGf,solv-DGu,solv > is only ~10 x too large in magnitude. This quantity should calculated accurately by APBS. How do your =20 parameters (radii, surface definitions, dielectric constants, etc.) =20 compare to the paper you're benchmarking against? Thanks, Nathan > Thanks again, > Steve > > I am including the .in files for the vacuum calculations. The =20 > aq .in files have not changed. > > In file for protein in vacuum: > read > mol pqr last_1.pdb.pqr > end > elec name 1 > mg-auto > dime 129 129 97 > cglen 82.9787 75.6908 64.4589 > fglen 68.8110 64.5240 57.9170 > cgcent mol 1 > fgcent mol 1 > mol 1 > lpbe > bcfl sdh > pdie 2 > sdie 2 > srfm smol > chgm spl2 > sdens 10.00 > srad 1.40 > swin 0.30 > temp 298.15 > gamma 0.105 > calcenergy comps > calcforce no > end > print energy 1 end > quit > > > in file for residue in vacuum: > read > mol pqr last_1.pdb.pqr > mol pqr last_1_res_1.pqr > end > elec name 1 > mg-auto > dime 129 129 97 > cglen 82.9787 75.6908 64.4589 > fglen 68.8110 64.5240 57.9170 > cgcent mol 1 > fgcent mol 1 > mol 1 > lpbe > bcfl sdh > pdie 2 > sdie 2 > srfm smol > chgm spl2 > sdens 10.00 > srad 1.40 > swin 0.30 > temp 298.15 > gamma 0.105 > calcenergy no > calcforce no > end > elec name 2 > mg-auto > dime 129 129 97 > cglen 82.9787 75.6908 64.4589 > fglen 68.8110 64.5240 57.9170 > cgcent mol 1 > fgcent mol 1 > mol 2 > lpbe > bcfl sdh > pdie 2 > sdie 2 > srfm smol > chgm spl2 > sdens 10.00 > srad 1.40 > swin 0.30 > temp 298.15 > gamma 0.105 > calcenergy comps > calcforce no > end > print energy 1 end > quit > > On Oct 1, 2006, at 5:13 PM, Nathan Baker wrote: > >> Hello -- >> >> Based on the input files you've included, it looks as if you're not >> correctly removing self-energies. =46rom your e-mail, it seems = you're >> interested in the difference in electrostatic energy between two >> configurations. Since the configurations are different, you can't >> rely on cancellation of self-energies between the two calculations. >> Instead, what you want to do is calculate solvation energies for each >> of the configurations and then take the difference of these solvation >> energies. This difference (the change in solvation energy due to un/ >> folding) can be added to the difference in Coulombic energy >> (electrostatic energy in a homogeneous dielectric) change to give the >> total electrostatic energy change. >> >> Does that make sense? >> >> Thanks, >> >> Nathan >> > -- Assistant Professor, Dept. of Biochemistry and Molecular Biophysics Center for Computational Biology, Washington University in St. Louis Web: http://cholla.wustl.edu/ |