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Temperature and pressure denaturation of chignolin: Folding and unfolding simulation by multibaric‐multithermal molecular dynamics method
Author(s) -
Okumura Hisashi
Publication year - 2012
Publication title -
proteins: structure, function, and bioinformatics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.699
H-Index - 191
eISSN - 1097-0134
pISSN - 0887-3585
DOI - 10.1002/prot.24125
Subject(s) - molecular dynamics , chemistry , enthalpy , denaturation (fissile materials) , thermodynamics , helix (gastropod) , crystallography , molecule , folding (dsp implementation) , protein folding , force field (fiction) , chemical physics , computational chemistry , physics , organic chemistry , ecology , biochemistry , quantum mechanics , biology , snail , electrical engineering , nuclear chemistry , engineering
A multibaric‐multithermal molecular dynamics (MD) simulation of a 10‐residue protein, chignolin, was performed. All‐atom model with the Amber parm99SB force field was used for the protein and the TIP3P model was used for the explicit water molecules. This MD simulation covered wide ranges of temperature between 260 and 560 K and pressure between 0.1 and 600 MPa and sampled many conformations without getting trapped in local‐minimum free‐energy states. Folding events to the native β‐hairpin structure occurred five times and unfolding events were observed four times. As the temperature and/or pressure increases, fraction of folded chignolin decreases. The partial molar enthalpy change Δ H and partial molar volume change Δ V of unfolding were calculated as Δ H = 24.1 ± 4.9 kJ/mol and Δ V = −5.6 ± 1.5 cm 3 /mol, respectively. These values agree well with recent experimental results. Illustrating typical local‐minimum free‐energy conformations, folding and unfolding pathways were revealed. When chignolin unfolds from the β‐hairpin structure, only the C terminus or both C and N termini open first. It may undergo an α‐helix or 3 10 ‐helix structure and finally unfolds to the extended structure. Difference of the mechanism between temperature denaturation and pressure denaturation is also discussed. Temperature denaturation is caused by making the protein transferred to a higher entropy state and making it move around more with larger space. The reason for pressure denaturation is that water molecules approach the hydrophobic residues, which are not well hydrated at the folded state, and some hydrophobic contacts are broken. Proteins 2012;. © 2012 Wiley Periodicals, Inc.