scholarly journals Protein Folding as a Resonance Phenomenon, with Folding Free Energies Determined by Protein-Hydration Shell Interactions

2017 ◽  
Vol 112 (3) ◽  
pp. 52a
Author(s):  
Sungchul Ji
2020 ◽  
Vol 22 (14) ◽  
pp. 7340-7347
Author(s):  
Akash Deep Biswas ◽  
Vincenzo Barone ◽  
Andrea Amadei ◽  
Isabella Daidone

An increase in protein hydration-shell density relative to that of the bulk is observed (in the range of 4–14%) for all studied proteins and this density-increment, which decreases for decreasing protein size, is caused by the protein size only.


2009 ◽  
Vol 96 (5) ◽  
pp. 1939-1943 ◽  
Author(s):  
S.E. Pagnotta ◽  
F. Bruni ◽  
R. Senesi ◽  
A. Pietropaolo

2007 ◽  
Vol 98 (13) ◽  
Author(s):  
R. Senesi ◽  
A. Pietropaolo ◽  
A. Bocedi ◽  
S. E. Pagnotta ◽  
F. Bruni

2016 ◽  
Vol 18 (40) ◽  
pp. 28175-28182 ◽  
Author(s):  
Sara Del Galdo ◽  
Andrea Amadei

In this paper we apply the computational analysis recently proposed by our group to characterize the solvation properties of a native protein in aqueous solution, and to four model aqueous solutions of globular proteins in their unfolded states thus characterizing the protein unfolded state hydration shell and quantitatively evaluating the protein unfolded state partial molar volumes.


2018 ◽  
Vol 551 ◽  
pp. 249-255 ◽  
Author(s):  
Satoshi Ajito ◽  
Mitsuhiro Hirai ◽  
Hiroki Iwase ◽  
Nobutaka Shimizu ◽  
Noriyuki Igarashi ◽  
...  

Biochemistry ◽  
1991 ◽  
Vol 30 (40) ◽  
pp. 9686-9697 ◽  
Author(s):  
Kim A. Sharp ◽  
Anthony Nicholls ◽  
Richard Friedman ◽  
Barry Honig

1993 ◽  
Vol 71 (9) ◽  
pp. 1368-1377 ◽  
Author(s):  
David A. Armstrong ◽  
Arvi Rauk ◽  
Dake Yu

Ab initio calculations are performed for [Formula: see text] and [Formula: see text] complexes for n = 0–5. For n = 0 and 1, the geometries of the complexes are optimized at the HF/6-31 + G* and MP2/6-31 + G* levels, and the energies are evaluated at the G2 level. For n = 2–5, the geometry optimizations and frequency calculations are carried out at the HF/6-31 + G* level, and the MP2/6-31 + G* energies are calculated at the HF optimized geometries. Basis set superposition errors are corrected by the Boys–Bernardi scheme at the HF/6-31 + G* level. The gas phase thermodynamic properties [Formula: see text] are evaluated as functions of temperature using standard statistical methods. Based on the calculated binding energies and the thermodynamic functions, the incremental changes in enthalpies and free energies, ΔHn and ΔGn, for the gas phase equilibria (H2O)n−1 M+ + H2O → (H2O)nM+ for M+ = NH4+ and NH3•+, are evaluated in comparison with the experimental data for [Formula: see text] the present results suggest conformations for the hydrated complexes observed in the experiments. The total free energy change for filling the first hydration shell is significantly more negative for NH3•+ than for NH4+.


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