Polyproline II helix is the preferred conformation for unfolded polyalanine in water

Does aqueous solvent discriminate among peptide conformers? To address this question, we computed the solvation free energy of a blocked, 12‐residue polyalanyl‐peptide in explicit water and analyzed its solvent structure. The peptide was modeled in each of 4 conformers: α‐helix, antiparallel β‐strand, parallel β‐strand, and polyproline II helix (PII). Monte Carlo simulations in the canonical ensemble were performed at 300 K using the CHARMM 22 forcefield with TIP3P water. The simulations indicate that the solvation free energy of PII is favored over that of other conformers for reasons that defy conventional explanation. Specifically, in these 4 conformers, an almost perfect correlation is found between a residue's solvent‐accessible surface area and the volume of its first solvent shell, but neither quantity is correlated with the observed differences in solvation free energy. Instead, solvation free energy tracks with the interaction energy between the peptide and its first‐shell water. An additional, previously unrecognized contribution involves the conformation‐dependent perturbation of first‐shell solvent organization. Unlike PII, β‐strands induce formation of entropically disfavored peptide:water bridges that order vicinal water in a manner reminiscent of the hydrophobic effect. The use of explicit water allows us to capture and characterize these dynamic water bridges that form and dissolve during our simulations. Proteins 2004. © 2004 Wiley‐Liss, Inc.

[1]  E. Baker,et al.  Hydrogen bonding in globular proteins. , 1984, Progress in biophysics and molecular biology.

[2]  L. Pratt,et al.  Hydration theory for molecular biophysics. , 2002, Advances in protein chemistry.

[3]  W G Richards,et al.  Computer-aided molecular design. , 1983, Endeavour.

[4]  T. Creamer,et al.  A survey of left‐handed polyproline II helices , 2008, Protein science : a publication of the Protein Society.

[5]  J. Dunitz The entropic cost of bound water in crystals and biomolecules. , 1994, Science.

[6]  E. Bandman,et al.  Analysis of the chicken fast myosin heavy chain family. Localization of isoform-specific antibody epitopes and regions of divergence. , 1992, Journal of molecular biology.

[7]  J. Owicki Optimization of Sampling Algorithms in Monte Carlo Calculations on Fluids , 1978 .

[8]  M Mezei,et al.  Structural chemistry of biomolecular hydration via computer simulation: the proximity criterion. , 1986, Methods in enzymology.

[9]  Mihaly Mezei,et al.  Unfolded state of polyalanine is a segmented polyproline II helix , 2004, Proteins.

[10]  C. Tanford Protein denaturation. , 1968, Advances in protein chemistry.

[11]  M. Mezei Calculation of solvation free-energy differences for large solute change from computer simulations with quadrature-based nearly linear thermodynamic integration , 1993 .

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

[13]  B. Lee,et al.  The interpretation of protein structures: estimation of static accessibility. , 1971, Journal of molecular biology.

[14]  M G Fried,et al.  Host-guest study of left-handed polyproline II helix formation. , 2001, Biochemistry.

[15]  S. Krimm,et al.  New chain conformations of poly(glutamic acid) and polylysine. , 1968, Biopolymers.

[16]  T. Creamer Left‐handed polyproline II helix formation is (very) locally driven , 1998, Proteins.

[17]  G. Rose,et al.  A simple model for polyproline II structure in unfolded states of alanine‐based peptides , 2002, Protein science : a publication of the Protein Society.

[18]  N. Metropolis,et al.  Equation of State Calculations by Fast Computing Machines , 1953, Resonance.

[19]  J. Brandts The Thermodynamics of Protein Denaturation. I. The Denaturation of Chymotrypsinogen , 1964 .

[20]  R. L. Baldwin,et al.  Energetics of the interaction between water and the helical peptide group and its role in determining helix propensities. , 2000, Proceedings of the National Academy of Sciences of the United States of America.

[21]  R. Srinivasan,et al.  The Flory isolated-pair hypothesis is not valid for polypeptide chains: implications for protein folding. , 2000, Proceedings of the National Academy of Sciences of the United States of America.

[22]  J. Flippen-Anderson,et al.  Aqueous channels within apolar peptide aggregates: solvated helix of the alpha-aminoisobutyric acid (Aib)-containing peptide Boc-(Aib-Ala-Leu)3-Aib-OMe.2H2O.CH3OH in crystals. , 1988, Proceedings of the National Academy of Sciences of the United States of America.

[23]  C. H. Walker The Hydrophobic Effect: Formation of Micelles and Biological Membranes , 1981 .

[24]  Edsall Jt,et al.  Water and proteins. I. The significance and structure of water; its interaction with electrolytes and non-electrolytes. , 1978 .

[25]  George D Rose,et al.  Polyproline II structure in a sequence of seven alanine residues , 2002, Proceedings of the National Academy of Sciences of the United States of America.

[26]  W. Kauzmann Some factors in the interpretation of protein denaturation. , 1959, Advances in protein chemistry.

[27]  N. Sreerama,et al.  Molecular dynamics simulations of polypeptide conformations in water: A comparison of α, β, and poly(pro)II conformations , 1999 .

[28]  L. Pauling,et al.  The structure of proteins; two hydrogen-bonded helical configurations of the polypeptide chain. , 1951, Proceedings of the National Academy of Sciences of the United States of America.

[29]  T. Creamer,et al.  Polyproline II helical structure in protein unfolded states: Lysine peptides revisited , 2002, Protein science : a publication of the Protein Society.

[30]  K. Dill,et al.  Hydrogen bonding in globular proteins. , 1992, Journal of molecular biology.

[31]  Peter Lykos,et al.  Computer Modeling of Matter , 1978 .

[32]  Distance-scaled Force Biased Monte Carlo Simulation for Solutions containing a Strongly Interacting Solute , 1991 .

[33]  R. L. Baldwin,et al.  Temperature dependence of the hydrophobic interaction in protein folding. , 1986, Proceedings of the National Academy of Sciences of the United States of America.

[34]  Mihaly Mezei,et al.  Studies on free energy calculations. I. Thermodynamic integration using a polynomial path , 1993 .

[35]  Mihaly Mezei Modified Proximity Criteria for the Analysis of the Solvation of a Polyfunctional Solute , 1988 .

[36]  J. Brandts The Thermodynamics of Protein Denaturation. II. A Model of Reversible Denaturation and Interpretations Regarding the Stability of Chymotrypsinogen , 1964 .

[37]  M. Mezei Direct Calculation of the Excess Free Energy of the Dense Lennard-Jones Fluid , 1989 .

[38]  R. L. Baldwin,et al.  Role of backbone solvation in determining thermodynamic β propensities of the amino acids , 2002, Proceedings of the National Academy of Sciences of the United States of America.

[39]  T. N. Bhat,et al.  The Protein Data Bank , 2000, Nucleic Acids Res..

[40]  R. Berry,et al.  Investigations into sequence and conformational dependence of backbone entropy, inter-basin dynamics and the Flory isolated-pair hypothesis for peptides. , 2003, Journal of molecular biology.

[41]  J. Onuchic,et al.  Pressure-induced protein-folding/unfolding kinetics. , 1999, Proceedings of the National Academy of Sciences of the United States of America.

[42]  Alexander D. MacKerell,et al.  All-atom empirical potential for molecular modeling and dynamics studies of proteins. , 1998, The journal of physical chemistry. B.

[43]  K. Sharp,et al.  Accurate Calculation of Hydration Free Energies Using Macroscopic Solvent Models , 1994 .

[44]  R. Raines,et al.  An electronic effect on protein structure , 2003, Protein science : a publication of the Protein Society.

[45]  Angel E. Garcia,et al.  Characterization of non-alpha helical conformations in Ala peptides , 2004 .

[46]  Christoph Weise,et al.  Do Bridging Water Molecules Dictate the Structure of a Model Dipeptide in Aqueous Solution , 2000 .

[47]  D. Chapman,et al.  The Hydrophobic Effect: Formation of Micelles and Biological Membranes (2nd Edition) , 1981 .

[48]  M. Mezei Polynomial path for the calculation of liquid state free energies from computer simulations tested on liquid water , 1992 .

[49]  T. Creamer,et al.  Determinants of the polyproline II helix from modeling studies. , 2002, Advances in protein chemistry.

[50]  R. L. Baldwin,et al.  Role of backbone solvation and electrostatics in generating preferred peptide backbone conformations: Distributions of phi , 2003, Proceedings of the National Academy of Sciences of the United States of America.