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Performance of hybrid methods for large‐scale unconstrained optimization as applied to models of proteins
Author(s) -
Das B.,
Meirovitch H.,
Navon I. M.
Publication year - 2003
Publication title -
journal of computational chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.907
H-Index - 188
eISSN - 1096-987X
pISSN - 0192-8651
DOI - 10.1002/jcc.10275
Subject(s) - hessian matrix , broyden–fletcher–goldfarb–shanno algorithm , preconditioner , function (biology) , mathematics , chemistry , computer science , algorithm , iterative method , computer network , asynchronous communication , evolutionary biology , biology
Energy minimization plays an important role in structure determination and analysis of proteins, peptides, and other organic molecules; therefore, development of efficient minimization algorithms is important. Recently, Morales and Nocedal developed hybrid methods for large‐scale unconstrained optimization that interlace iterations of the limited‐memory BFGS method (L‐BFGS) and the Hessian‐free Newton method (Computat Opt Appl 2002, 21, 143–154). We test the performance of this approach as compared to those of the L‐BFGS algorithm of Liu and Nocedal and the truncated Newton (TN) with automatic preconditioner of Nash, as applied to the protein bovine pancreatic trypsin inhibitor (BPTI) and a loop of the protein ribonuclease A. These systems are described by the all‐atom AMBER force field with a dielectric constant ϵ = 1 and a distance‐dependent dielectric function ϵ = 2 r , where r is the distance between two atoms. It is shown that for the optimal parameters the hybrid approach is typically two times more efficient in terms of CPU time and function/gradient calculations than the two other methods. The advantage of the hybrid approach increases as the electrostatic interactions become stronger, that is, in going from ϵ = 2 r to ϵ = 1, which leads to a more rugged and probably more nonlinear potential energy surface. However, no general rule that defines the optimal parameters has been found and their determination requires a relatively large number of trial‐and‐error calculations for each problem. © 2003 Wiley Periodicals, Inc. J Comput Chem 24: 1222–1231, 2003

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