Thermodynamics of protein-peptide interactions in the ribonuclease-S system studied by molecular dynamics and free energy calculations.

Hydrophobic interactions between the S-peptide and S-protein in the ribonuclease-S complex are probed using molecular dynamics simulations and free energy calculations. Three successive mutations at the buried position Met13 are simulated: Met----Leu, Leu----Ile, and Ile----Val, for which X-ray structures and experimental thermodynamic data are available. The calculations give theoretical estimates of the changes in binding free energies associated with these mutations. The calculated free energy differences are small (0-1.6 kcal/mol), in agreement with experiment. However the simulated structures deviate significantly from the experimental ones (mean deviation approximately 1.5-2 A), and a large uncertainty in the calculated free energies (1-2 kcal/mol) arises from the multiple minimum problem. Indeed, multiple conformations are available to the side chains around the mutation site, and the sampling of dihedral rotamer transitions is limited, despite long simulations. Fluctuations within each local minimum give rise to a small statistical error. However the uncertainty due to multiple conformations is much greater than the uncertainty due to random statistical errors. In our work, an artificial cancellation of errors arose because we studied conformations of the RNase complex and of the S-peptide that were very similar. In general, the criterion for a precise simulation is not merely to reduce the random statistical error, as has been suggested, but rather to sample all the important local minima along the mutation pathway, and to reduce the statistical error for each one. Our calculations suggest that the packing changes associated with the mutations are energetically small and localized, and largely cancel when the complex and the S-peptide are compared. Solvation of the methionine side chain partial charges in the S-peptide and the complex appear to be energetically equivalent, so that removing them (as in Met13----Leu, Ile, Val) does not affect binding. Enthalpy and entropy changes could not be estimated reliably.

[1]  M. Karplus,et al.  Active site dynamics in protein molecules: A stochastic boundary molecular‐dynamics approach , 1985, Biopolymers.

[2]  William L. Jorgensen,et al.  Free energy calculations: a breakthrough for modeling organic chemistry in solution , 1989 .

[3]  J. A. McCammon,et al.  Dynamics and Design of Enzymes and Inhibitors. , 1986 .

[4]  W. L. Jorgensen Free energy calculations: a breakthrough for modeling organic chemistry in solution , 1989 .

[5]  P. A. Bash,et al.  Calculation of the relative change in binding free energy of a protein-inhibitor complex. , 1987, Science.

[6]  C. Brooks Thermodynamic calculations on biological molecules , 1988 .

[7]  G. Ciccotti,et al.  Numerical Integration of the Cartesian Equations of Motion of a System with Constraints: Molecular Dynamics of n-Alkanes , 1977 .

[8]  M. Karplus,et al.  Deformable stochastic boundaries in molecular dynamics , 1983 .

[9]  H. Rüterjans,et al.  NMR-studies on the structure of the active site of pancreatic ribonuclease A. , 1969, European journal of biochemistry.

[10]  H. Berendsen,et al.  THERMODYNAMICS OF CAVITY FORMATION IN WATER - A MOLECULAR-DYNAMICS STUDY , 1982 .

[11]  A. J. Stam,et al.  Estimation of statistical errors in molecular simulation calculations , 1986 .

[12]  M. Karplus,et al.  Hidden thermodynamics of mutant proteins: a molecular dynamics analysis. , 1989, Science.

[13]  M. Levitt,et al.  Conformation of amino acid side-chains in proteins. , 1978, Journal of molecular biology.

[14]  W. Lim,et al.  Mutational analysis of protein stability , 1992, Current Biology.

[15]  D. Wallace,et al.  Statistical errors in molecular dynamics averages , 1985 .

[16]  H. Berendsen,et al.  Molecular dynamics with coupling to an external bath , 1984 .

[17]  James Andrew McCammon,et al.  Ligand-receptor interactions , 1984, Comput. Chem..

[18]  D. Walters,et al.  Tautomeric states of the histidine residues of bovine pancreatic ribonuclease A. Application of carbon 13 nuclear magnetic resonance spectroscopy. , 1980, The Journal of biological chemistry.

[19]  S. Moore,et al.  12 Pancreatic Ribonuclease , 1982 .

[20]  F. Richards,et al.  Crystallographic structures of ribonuclease S variants with nonpolar substitution at position 13: packing and cavities. , 1993, Biochemistry.

[21]  B. Matthews,et al.  Response of a protein structure to cavity-creating mutations and its relation to the hydrophobic effect. , 1992, Science.

[22]  A Tropsha,et al.  Application of free energy simulations to the binding of a transition-state-analogue inhibitor to HIV protease. , 1992, Protein engineering.

[23]  J. Lenstra,et al.  The aromatic residues of bovine pancreatic ribonuclease studied by 1H nuclear magnetic resonance. , 1979, European journal of biochemistry.

[24]  Peter A. Kollman,et al.  A new method for carrying out free energy perturbation calculations: Dynamically modified windows , 1989 .

[25]  J M Sturtevant,et al.  Heat capacity changes for protein-peptide interactions in the ribonuclease S system. , 1992, Biochemistry.

[26]  H. Rüterjans,et al.  Proton-magnetic-resonance studies of complexes of pancreatic ribonuclease A with pyrimidine and purine nucleotides. , 1974, European journal of biochemistry.

[27]  F M Richards,et al.  Refinement of the crystal structure of ribonuclease S. Comparison with and between the various ribonuclease A structures. , 1994, Biochemistry.

[28]  J. Neira,et al.  Sequential 1H-NMR assignment and solution structure of bovine pancreatic ribonuclease A. , 1989, European journal of biochemistry.

[29]  Thomas E. Creighton,et al.  Stability of folded conformations , 1991 .

[30]  Jay W. Ponder,et al.  Tertiary Templates for Proteins Use of Packing Criteria in the Enumeration of Allowed Different Structural Classes Sequences , 1987 .

[31]  J. Neira,et al.  3D structure of bovine pancreatic ribonuclease A in aqueous solution: An approach to tertiary structure determination from a small basis of1H NMR NOE correlations , 1991, Journal of biomolecular NMR.

[32]  U. Singh,et al.  A NEW FORCE FIELD FOR MOLECULAR MECHANICAL SIMULATION OF NUCLEIC ACIDS AND PROTEINS , 1984 .

[33]  R. Zwanzig High‐Temperature Equation of State by a Perturbation Method. I. Nonpolar Gases , 1954 .

[34]  T. Alber,et al.  Mutational effects on protein stability. , 1989, Annual review of biochemistry.

[35]  S. Shall,et al.  Structure of Ribonuclease , 1967, Nature.

[36]  A Wlodawer,et al.  Nuclear magnetic resonance and neutron diffraction studies of the complex of ribonuclease A with uridine vanadate, a transition-state analogue. , 1985, Biochemistry.

[37]  F. Cohen,et al.  Hydrogen bonds involving sulfur atoms in proteins , 1991, Proteins.

[38]  T C Terwilliger,et al.  Influence of interior packing and hydrophobicity on the stability of a protein. , 1989, Science.

[39]  F M Richards,et al.  The structure of ribonuclease-S at 3.5 A resolution. , 1967, The Journal of biological chemistry.

[40]  P. Kraulis A program to produce both detailed and schematic plots of protein structures , 1991 .

[41]  M Karplus,et al.  Simulation analysis of the stability mutant R96H of T4 lysozyme. , 1991, Biochemistry.

[42]  W E Stites,et al.  Contributions of the large hydrophobic amino acids to the stability of staphylococcal nuclease. , 1990, Biochemistry.

[43]  F M Richards,et al.  Areas, volumes, packing and protein structure. , 1977, Annual review of biophysics and bioengineering.

[44]  H. Scheraga,et al.  Proton NMR assignments and regular backbone structure of bovine pancreatic ribonuclease A in aqueous solution. , 1989, Biochemistry.

[45]  D S Moss,et al.  Segmented anisotropic refinement of bovine ribonuclease A by the application of the rigid-body TLS model. , 1989, Acta crystallographica. Section A, Foundations of crystallography.

[46]  L. Verlet Computer "Experiments" on Classical Fluids. I. Thermodynamical Properties of Lennard-Jones Molecules , 1967 .

[47]  W. L. Jorgensen,et al.  Comparison of simple potential functions for simulating liquid water , 1983 .

[48]  C. Brooks,et al.  Calculation of free energy surfaces using the methods of thermodynamic perturbation theory , 1987 .

[49]  H. Witzel The Function of the Pyrimidine Base in the Ribonuclease Reaction1 , 1963 .

[50]  H. Scheraga,et al.  Assignment of the histidine peaks in the nuclear magnetic resonance spectrum of ribonuclease. , 1968, Proceedings of the National Academy of Sciences of the United States of America.

[51]  J. Cohen,et al.  Specific peptide-protein interactions in the ribonuclease S' system studied by 13C nuclear magnetic resonance spectroscopy with selectively 13C-enriched peptides. , 1979, The Journal of biological chemistry.

[52]  J. Kirkwood Statistical Mechanics of Fluid Mixtures , 1935 .

[53]  F. Richards,et al.  24 Bovine Pancreatic Ribonuclease , 1971 .

[54]  F. Richards,et al.  Thermodynamics of protein-peptide interactions in the ribonuclease S system studied by titration calorimetry. , 1990, Biochemistry.

[55]  A. Schechter,et al.  NUCLEAR MAGNETIC RESONANCE STUDIES OF A RIBONUCLEASE‐DINUCLEOSIDE PHOSPHONATE COMPLEX AND THEIR IMPLICATIONS FOR THE MECHANISM OF THE ENZYME , 1973, Annals of the New York Academy of Sciences.

[56]  M Karplus,et al.  Active site dynamics of ribonuclease. , 1985, Proceedings of the National Academy of Sciences of the United States of America.

[57]  A Wlodawer,et al.  The refined crystal structure of ribonuclease A at 2.0 A resolution. , 1982, The Journal of biological chemistry.

[58]  Peter A. Kollman,et al.  Free energy calculations on protein stability: Thr-157 .fwdarw. Val-157 mutation of T4 lysozyme , 1989 .

[59]  C Etchebest,et al.  Conformational and helicoidal analysis of the molecular dynamics of proteins: “Curves,” dials and windows for a 50 psec dynamic trajectory of BPTI , 1990, Proteins.

[60]  T Tsujita,et al.  Dependence of conformational stability on hydrophobicity of the amino acid residue in a series of variant proteins substituted at a unique position of tryptophan synthase alpha subunit. , 1987, Proceedings of the National Academy of Sciences of the United States of America.

[61]  W. Lim,et al.  The role of internal packing interactions in determining the structure and stability of a protein. , 1991, Journal of molecular biology.

[62]  W. L. Jorgensen,et al.  The OPLS [optimized potentials for liquid simulations] potential functions for proteins, energy minimizations for crystals of cyclic peptides and crambin. , 1988, Journal of the American Chemical Society.

[63]  J. Andrew McCammon,et al.  Mass and step length optimization for the calculation of equilibrium properties by molecular dynamics simulation , 1990 .

[64]  A. Fersht,et al.  Energetics of complementary side-chain packing in a protein hydrophobic core. , 1989, Biochemistry.

[65]  J Hermans,et al.  Microfolding: Conformational probability map for the alanine dipeptide in water from molecular dynamics simulations , 1988, Proteins.

[66]  A. W. Hanson,et al.  The three-dimensional structure of ribonuclease-S. Interpretation of an electron density map at a nominal resolution of 2 A. , 1970, The Journal of biological chemistry.

[67]  S J Wodak,et al.  Contribution of the hydrophobic effect to protein stability: analysis based on simulations of the Ile-96----Ala mutation in barnase. , 1991, Proceedings of the National Academy of Sciences of the United States of America.

[68]  D. Beveridge,et al.  Free energy via molecular simulation: applications to chemical and biomolecular systems. , 1989, Annual review of biophysics and biophysical chemistry.

[69]  J. Markley Correlation proton magnetic resonance studies at 250 MHz of bovine pancreatic ribonuclease. I. Reinvestigation of the histidine peak assignments. , 1975, Biochemistry.

[70]  G. Petsko,et al.  Ribonuclease structure and catalysis: crystal structure of sulfate-free native ribonuclease A at 1.5-A resolution. , 1987, Biochemistry.