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Effect of stereochemical constraints on the structural properties of folded proteins

Jack A. Logan1,*, Jacob Sumner2,3,*, Alex T. Grigas2,3, Mark D. Shattuck4, and Corey S. O'Hern5,2,3,6,7

  • 1Department of Mechanical Engineering, Yale University, New Haven, Connecticut 06520, USA
  • 2Graduate Program in Computational Biology and Bioinformatics, Yale University, New Haven, Connecticut 06520, USA
  • 3Integrated Graduate Program in Physical and Engineering Biology, Yale University, New Haven, Connecticut 06520, USA
  • 4Benjamin Levich Institute and Physics Department, The City College of New York, New York, New York 10031, USA
  • 5Department of Mechanical Engineering, Yale University, New Haven, Connecticut 06520, USA
  • 6Department of Physics, Yale University, New Haven, Connecticut 06520, USA
  • 7Department of Applied Physics, Yale University, New Haven, Connecticut 06520, USA

  • *These authors contributed equally to this work.

Phys. Rev. E 112, 054405 – Published 6 November, 2025

DOI: https://doi.org/10.1103/9wf9-ywhw

Abstract

Proteins are composed of chains of amino acids that fold into complex three-dimensional structures. Several key features, such as the radius of gyration, fraction of core amino acids fcore, packing fraction 〈ϕ〉 of core amino acids, and structure factor S(q) define the structure of folded proteins. It is well-known that folded proteins are compact with a radius of gyration Rg(N)∼Nν that obeys power-law scaling with the number of amino acids N and ν∼1/3, fcore≈0.09, and 〈ϕ〉≈0.55. We also investigate the internal scaling of the radius of gyration Rg(n) versus the chemical separation n between amino acids for subchains of length n and show that it does not obey simple power-law scaling with ν∼1/3. Instead, Rg(n)∼nν1,2 with a larger exponent ν1>1/3 for small n and a smaller exponent ν2<1/3 for large n. To develop a minimal model for proteins that recapitulates these defining structural features, we carry out collapse simulations for a series of coarse-grained models with increasing complexity. We show that a model, which coarse-grains amino acids into a single spherical backbone bead and several variable-sized side-chain beads and enforces bend- and dihedral-angle constraints for the backbone, recapitulates Rg(n), fcore, 〈ϕ〉, and S(q) for more than 2500 x-ray crystal structures of proteins.

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