Reviews in Computational Chemistry Volume 18

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xxiv Contributors to Previous Volumes Jan Almlöf and Odd Gropen,* Relativistic Effects in Chemistry. Donald B. Chesnut, The Ab Initio Computation of Nuclear Magnetic Resonance Chemical Shielding. Volume 9 (1996) James R. Damewood Jr., Peptide Mimetic Design with the Aid of Computational Chemistry. T. P. Straatsma, Free Energy by Molecular Simulation. Robert J. Woods, The Application of Molecular Modeling Techniques to the Determination of Oligosaccharide Solution Conformations. Ingrid Pettersson and Tommy Liljefors, Molecular Mechanics Calculated Conformational Energies of Organic Molecules: A Comparison of Force Fields. Gustavo A. Arteca, Molecular Shape Descriptors. Volume 10 (1997) Richard Judson, y Genetic Algorithms and Their Use in Chemistry. Eric C. Martin, David C. Spellmeyer, Roger E. Critchlow Jr., and Jeffrey M. Blaney, Does Combinatorial Chemistry Obviate Computer-Aided Drug Design? Robert Q. Topper, Visualizing Molecular Phase Space: Nonstatistical Effects in Reaction Dynamics. Raima Larter and Kenneth Showalter, Computational Studies in Nonlinear Dynamics. Stephen J. Smith and Brian T. Sutcliffe, The Development of Computational Chemistry in the United Kingdom. *Address: Institute of Mathematical and Physical Sciences, University of Tromsø, N-9037 Tromsø, Norway (Electronic mail: oddg@chem.uit.no). y Current address: Genaissance Pharmaceuticals, Five Science Park, New Haven, Connecticut 06511 (Electronic mail: r.judson@genaissance.com).
Volume 11 (1997) Mark A. Murcko, Recent Advances in Ligand Design Methods. David E. Clark,* Christopher W. Murray, and Jin Li, Current Issues in De Novo Molecular Design. Tudor I. Oprea y and Chris L. Waller, Theoretical and Practical Aspects of Three-Dimensional Quantitative Structure–Activity Relationships. Giovanni Greco, Ettore Novellino, and Yvonne Connolly Martin, Approaches to Three-Dimensional Quantitative Structure–Activity Relationships. Pierre-Alain Carrupt, Bernard Testa, and Patrick Gaillard, Computational Approaches to Lipophilicity: Methods and Applications. Ganesan Ravishanker, Pascal Auffinger, David R. Langley, Bhyravabhotla Jayaram, Matthew A. Young, and David L. Beveridge, Treatment of Counterions in Computer Simulations of DNA. Donald B. Boyd, Appendix: Compendium of Software and Internet Tools for Computational Chemistry. Volume 12 (1998) Contributors to Previous Volumes xxv Hagai Meirovitch, z Calculation of the Free Energy and the Entropy of Macromolecular Systems by Computer Simulation. Ramzi Kutteh and T. P. Straatsma, Molecular Dynamics with General Holonomic Constraints and Application to Internal Coordinate Constraints. John C. Shelley } and Daniel R. Bérard, Computer Simulation of Water Physisorption at Metal–Water Interfaces. *Current address: Computer-Aided Drug Design, Argenta Discovery Ltd., 8/9 Spire Green Centre, Flex Meadow, Harlow, Essex, CM19 5TR, United Kingdom (Electronic mail: david.clark@argentadiscovery.com). y Current address: Office of Biocomputing, University of New Mexico School of Medicine, 915 Camino de Salud NE, Albuquerque, New Mexico 87131 (Electronic mail: toprea@salud.unm.edu). z Current address: Department of Molecular Genetics & Biochemistry, School of Medicine, University of Pittsburgh, Pittsburgh, Pennsylvania 15213 (Electronic mail: hagaim@pitt. edu). } Current address: Schrödinger, Inc., 1500 S.W. First Avenue, Suite 1180, Portland, Oregon 97201 (Electronic mail: jshelley@schrodinger.com).
Page 1 and 2: Reviews in Computational Chemistry
Page 3 and 4: Kenny B. Lipkowitz Department of Ch
Page 5 and 6: vi Preface three-dimensional struct
Page 7 and 8: viii Preface some descriptors and i
Page 9 and 10: Epilogue and Dedication My associat
Page 11 and 12: Contents 1. Clustering Methods and
Page 13 and 14: Contents xv Electron Transfer in Po
Page 15 and 16: Contributors John M. Barnard, Barna
Page 17 and 18: Contributors to Previous Volumes *
Page 19 and 20: Volume 3 (1992) Tamar Schlick, Opti
Page 21: Volume 7 (1996) Geoffrey M. Downs a
Page 25 and 26: T. Daniel Crawford* and Henry F. Sc
Page 27 and 28: Topics Covered in Volumes 1-18 * Ab
Page 29 and 30: Reviews in Computational Chemistry
Page 31 and 32: 2 Clustering Methods and Their Uses
Page 39 and 40: 10 Clustering Methods and Their Use
Page 71 and 72: 42 The Use of Scoring Functions in
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44 The Use of Scoring Functions in
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Table 1 Reference List for the Most
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CHAPTER 3 Potentials and Algorithms
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Vn (1 + cos(nω + γ)) 2 K θ (θ
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are modified by their environment w
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Table 1 Polarizability Parameters f
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The polarizable point dipole models
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two to three orders of magnitude sl
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M i z i + q i d i k i and shell cha
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Shell Models 103 on estimates of sh
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minimization can be replaced by mor
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The energy required to create a cha
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for all i ði:e:; 8 iÞ: @U @qi l
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where we have used q Cl ¼ qNa. The
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Electronegativity Equalization Mode
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Electronegativity Equalization Mode
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of N molecules is taken as a Hartre
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is treated using variable charges.
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water have been developed, includin
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Applications 123 classical and rigi
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developing polarizable models. A va
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Comparison of the Polarization Mode
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negligible errors in such propertie
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ecome significant at field strength
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noteworthy in this regard because t
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References 135 9. P. Cieplak and P.
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References 137 48. E. L. Pollock an
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References 139 Computational Chemis
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References 141 139. J. Hinze and H.
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References 143 178. J. J. P. Stewar
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References 145 216. M. W. Mahoney a
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CHAPTER 4 New Developments in the T
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Introduction 149 applications). For
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FCWD(∆E ) FCWD(0) ∆E = 0 ∆E
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Introduction 153 Equations [6]-[12]
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Paradigm of Free Energy Surfaces 15
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Paradigm of Free Energy Surfaces 15
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In Eqs. [18] and [19], F0i is the e
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where ‘‘þ’’ and ‘‘ ’
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is, however, small for the usual co
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solute-solvent coupling through the
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where Z is the electrode overpotent
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energy surfaces of ET. 33,50-56 It
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This result indicates a fundamental
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βF i (X ) 40 20 0 −20 1 2 βλ 1
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Table 1 Main Features of the Two-Pa
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and Hss ¼ U rep ss 1 2 X j;k ðmj
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λ i /eV 4 3 2 1 0 0 10 20 30 40 Bo
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the width/Stokes shift relation (Eq
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Table 3 Mapping of the Q Model on S
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This situation is of course not sat
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F ± (Y ad )/λ I 0.8 0.4 0 −0.4
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it by choosing the GMH basis set 7
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Anharmonic higher order terms gain
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of the radiation is the perturbatio
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individual vibrational excitations
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m 12 /D 6 5.5 5 4.5 4 3.5 17 18 19
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In Eq. [144], the coordinates Y km
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ε/M −1 cm −1 4000 2000 0 analy
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βσ 2 /10 3 cm −1 14 12 10 8 Opt
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0.2 0.1 0 12 16 20 24 28 32 The app
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References 207 7. M. D. Newton, Adv
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References 209 59. R. Kubo and Y. T
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