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INTERACTIONS IN PROTEINS AND THEIR ROLE IN STRUCTURE FORMATION
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Levels of protein structure organization
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Dominant forces in protein folding Electrostatic forces Hydrogen bonding and van der Waals interactions Intrinsic properties Hydrophobic forces Conformational entropy (opposes folding)
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Can we say that there are „dominant” forces in protein folding? Hardly. Proteins are only marginally stable (5 – 20 k B T/molecule). For comparison: water-water H-bond has about 5 kcal/mol (9 k B T/molecule) Consequently, even the tiniest force cannot be ignored. However, different types of interactions play different role Hydrophobic interaction: compactness Local interactions: chain stiffness Hydrogen bonds: architecture
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Local and nonlocal interactions
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Long-range vs. short-range interactions n<=3: long range interactions n>3: short-range interactions Long-range: electrostatic (charge-charge, charge-dipole, and dipole-dipole) interactions Short-range: van der Waals repulsion and attraction, hydrophobic interactions
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Electrostatic interactions
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Lots of like-charges (e.g., side-chain ionization by pH decrease/increase) destabilize protein structure Increase of ionic strength destabilizes protein structure 5 – 10 kcal/mol / counter-ion (salt-bridge) pair A protein contains only a small number of salt bridges, mainly located on the surface (nevertheless, they can be essential).
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Example of a surface salt bridge: salt bridge triad between Asp8, Asp12 and Arg110 on the surface of barnase
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Replacement of charged residues with hydrophobic residues can increase the stability by 3-4 kcal/mol. Example: ARC repressor Wild type: salt triad between R31, E36, and R40 Mutant: hydrophobic packing between M31, Y36, and L40
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Potentials of mean force
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Maksimiak et al., J.Phys.Chem. B, 107, 13496-13504 (2003)
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Masunov & Lazaridis, J.Am.Chem.Soc., 125, 1722-1730 (2003)
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Hydrogen-bonding and van der Waals forces
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A w +B w A n +B n (AB) w (AB) n G 1 =-2.40 kcal/mol G 3 =+3.10 kcal/mol G 4 =+0.62 kcal/mol G 3 =+3.10 kcal/mol Free energies of N-methylamide dimerization in water (w) and CCl 4 (n) solution and transfer between these solvents
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Local interactions are largely determined by Ramachandran map
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Conformations of a terminally-blocked amino-acid residue C 7 eq C 7 ax E Zimmerman, Pottle, Nemethy, Scheraga, Macromolecules, 10, 1-9 (1977)
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Energy maps of Ac-Ala-NHMe and Ac-Gly-AHMe obtained with the ECEPP/2 force field
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Energy curve of Ac-Pro-NHMe obtained with the ECEPP/2 force field L-Pro -68 o
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Energy minima of therminally-blocked alanine with the ECEPP/2 force field
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Hydrophobic forces
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Sobolewski et al., J.Phys.Chem., 111, 10765-10744 (2008)
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Dependence of the PMF and cavity contribution to the PMF of two methane molecules on temperature (Sobolewski et al., PEDS, 22, 547-552 (2009)
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S. Miyazawa & R.L. Jernigan, R. L. 1985. Estimation of effective interresidue contact energies from protein crystal structures: quasi-chemical approximation. Macromolecules, 18:534-552, 1985.
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CMFILVWYAGTSQNEDHRKP P K R H D E N Q S T G A Y W V L I F M C Color map of the MJ table
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Conformational entropy
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