3 Publications
Next
3.1 Papers
Section Intro | Molecular modeling | Bioinformatics | docking | Methods and algorithms | Applications | Chronological list

3.1.6 Chronological list
Section Contents | ref 1 | ref 2 | ref 3 | ref 4 | ref 5 | ref 6 | ref 7 | ref 8 | ref 9 | ref 10 | ref 11 | ref 12 | ref 13 | ref 14 | ref 15 | ref 16 | ref 17 | ref 18 | ref 19 | ref 20 | ref 21 | ref 22 | ref 23 | ref 24 | ref 25 | ref 26 | ref 27 | ref 28 | ref 29 | ref 30 | ref 31 | ref 32 | ref 33 | ref 34 | ref 35 | ref 36 | ref 37 | ref 38 | ref 39 | ref 40 | ref 41 | ref 42 | ref 43 | ref 44 | ref 45 | ref 46 | ref 47 | ref 48 | ref 49 | ref 50 | ref 51 | ref 52 | ref 53 | ref 54 | ref 55 | ref 56 | ref 57 | ref 58 | ref 59 | ref 60 | ref 61 | ref 62 | ref 63 | ref 64 | ref 65 | ref 66 | ref 67 | ref 68 | ref 69 | ref 70 | ref 71 | ref 72 | ref 73 | ref 74 | ref 75 | ref 76 | ref 77 | ref 78 | ref 79 | ref 80 | ref 81 | ref 82 | ref 83 | in press

3.1.6.30 Abagyan, R.A., and Totrov, M.M. (1994). Biased Probability Monte Carlo Conformational Searches and Electrostatic Calculations for Peptides and Proteins. J. Mol. Biol., 235, 983-1002

Two major components are required for a successful prediction of the three-dimensional structure of peptides and proteins: an efficient global optimization procedure which is capable of finding an appropriate local minimum for the strongly anisotropic function of hundreds of variables, and a set of free energy components for a protein molecule in solution which are computationally inexpensive enough to be used in the search procedure, yet sufficiently accurate to ensure the uniqueness of the native conformation. We here found an efficient way to make a random step in a Monte Carlo procedure given knowledge of the energy or statistical properties of conformational subspaces (e.g. phi-psi zones or side-chain torsion angles). This biased probability Monte Carlo (BPMC) procedure randomly selects the subspace first, then makes a step to a new random position independent of the previous position, but according to the predefined continuous probability distribution. The random step is followed by a local minimization in torsion angle space. The positions, sizes and preferences for high-probability zones on phi-psi maps and chi-angle maps were calculated for different residue types from the representative set of 191 and 161 protein 3D-structures, respectively. A fast and precise method to evaluate the electrostatic energy of a protein in solution is developed and combined with the BPMC procedure. The method is based on the modified spherical image charge approximation, efficiently projected onto a molecule of arbitrary shape. Comparison with the finite-difference solutions of the Poisson-Boltzmann equation shows high accuracy for our approach. The BPMC procedure is applied successfully to the structure prediction of 12- and 16-residue synthetic peptides and the determination of protein structure from NMR data, with the immunoglobulin binding domain of streptococcal protein G as an example. The BPMC runs display much better convergence properties than the non-biased simulations. The advantage of a true global optimization procedure for NMR structure determination is its ability to cope with local minima originating from data errors and ambiguities in NMR data.