TY - JOUR
T1 - Fast pressure-jump all-atom simulations and experiments reveal site-specific protein dehydration-folding dynamics
AU - Prigozhin, Maxim B.
AU - Zhang, Yi
AU - Schulten, Klaus
AU - Gruebele, Martin
AU - Pogorelov, Taras V.
N1 - We thank D. E. Shaw Research (DESR) for providing MD data for λ6–85 and α3D, and Dr. Anna Jean Wirth for assistance with setting up the P-jump. Anton 2 computer time was provided by the Pittsburgh Supercomputing Center (PSC) through Grant R01GM116961 from the NIH. The Anton 2 machine at the PSC was generously made available by DESR. We also thank DESR for providing access to the simulation data. This work was supported by NIH Grants R01GM093318 (to M.G.) and 9P41GM104601 (to K.S.). M.B.P. was supported by the Howard Hughes Medical Institute International Student Research Fellowship and the Helen Hay Whitney Foundation Postdoctoral Fellowship.
ACKNOWLEDGMENTS. We thank D. E. Shaw Research (DESR) for providing MD data for λ6–85 and α3D, and Dr. Anna Jean Wirth for assistance with setting up the P-jump. Anton 2 computer time was provided by the Pittsburgh Supercomputing Center (PSC) through Grant R01GM116961 from the NIH. The Anton 2 machine at the PSC was generously made available by DESR. We also thank DESR for providing access to the simulation data. This work was supported by NIH Grants R01GM093318 (to M.G.) and 9P41GM104601 (to K.S.). M.B.P. was supported by the Howard Hughes Medical Institute International Student Research Fellowship and the Helen Hay Whitney Foundation Postdoctoral Fellowship.
PY - 2019
Y1 - 2019
N2 - As theory and experiment have shown, protein dehydration is a major contributor to protein folding. Dehydration upon folding can be characterized directly by all-atom simulations of fast pressure drops, which create desolvated pockets inside the nascent hydrophobic core. Here, we study pressure-drop refolding of three λ-repressor fragment (λ 6 – 85 ) mutants computationally and experimentally. The three mutants report on tertiary structure formation via different fluorescent helix–helix contact pairs. All-atom simulations of pressure drops capture refolding and unfolding of all three mutants by a similar mechanism, thus validating the non-perturbative nature of the fluorescent contact probes. Analysis of simulated interprobe distances shows that the α-helix 1–3 pair distance displays a slower characteristic time scale than the 1–2 or 3–2 pair distance. To see whether slow packing of α-helices 1 and 3 is reflected in the rate-limiting folding step, fast pressure-drop relaxation experiments captured refolding on a millisecond time scale. These experiments reveal that refolding monitored by 1–3 contact formation indeed is much slower than when monitored by 1–2 or 3–2 contact formation. Unlike the case of the two-state folder [three–α-helix bundle (α 3 D)], whose drying and core formation proceed in concert, λ 6 – 85 repeatedly dries and rewets different local tertiary contacts before finally forming a solvent-excluded core, explaining the non–two-state behavior observed during refolding in molecular dynamics simulations. This work demonstrates that proteins can explore desolvated pockets and dry globular states numerous times before reaching the native conformation.
AB - As theory and experiment have shown, protein dehydration is a major contributor to protein folding. Dehydration upon folding can be characterized directly by all-atom simulations of fast pressure drops, which create desolvated pockets inside the nascent hydrophobic core. Here, we study pressure-drop refolding of three λ-repressor fragment (λ 6 – 85 ) mutants computationally and experimentally. The three mutants report on tertiary structure formation via different fluorescent helix–helix contact pairs. All-atom simulations of pressure drops capture refolding and unfolding of all three mutants by a similar mechanism, thus validating the non-perturbative nature of the fluorescent contact probes. Analysis of simulated interprobe distances shows that the α-helix 1–3 pair distance displays a slower characteristic time scale than the 1–2 or 3–2 pair distance. To see whether slow packing of α-helices 1 and 3 is reflected in the rate-limiting folding step, fast pressure-drop relaxation experiments captured refolding on a millisecond time scale. These experiments reveal that refolding monitored by 1–3 contact formation indeed is much slower than when monitored by 1–2 or 3–2 contact formation. Unlike the case of the two-state folder [three–α-helix bundle (α 3 D)], whose drying and core formation proceed in concert, λ 6 – 85 repeatedly dries and rewets different local tertiary contacts before finally forming a solvent-excluded core, explaining the non–two-state behavior observed during refolding in molecular dynamics simulations. This work demonstrates that proteins can explore desolvated pockets and dry globular states numerous times before reaching the native conformation.
KW - Molecular dynamics simulation
KW - Pressure jump
KW - Protein solvation dynamics
UR - https://www.scopus.com/pages/publications/85063277538
UR - https://www.scopus.com/pages/publications/85063277538#tab=citedBy
U2 - 10.1073/pnas.1814927116
DO - 10.1073/pnas.1814927116
M3 - Article
C2 - 30837309
AN - SCOPUS:85063277538
SN - 0027-8424
VL - 116
SP - 5356
EP - 5361
JO - Proceedings of the National Academy of Sciences of the United States of America
JF - Proceedings of the National Academy of Sciences of the United States of America
IS - 12
ER -