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Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems
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Mutational -value analysis of the folding kinetics Modeling -values for -helices Modeling -values for small -sheet proteins Overview
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Protein folding problems The structure problem: In which native structure does a given sequence fold? The kinetics problem: How does a protein fold into its structure?
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How does a protein fold? The ”old view”: Metastable folding intermediates guide a protein into its native structure The Levinthal paradox: How does a protein find its folded conformation as ”needle in the haystack“? The ”new view”: Many small proteins fold without detectable intermediates (2-state proteins)
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2-state folding: Single molecules Donor and acceptor dyes at chain ends Schuler et al., Nature 2002 State-dependent transfer efficiency
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2-state folding: Protein ensemble rapid mixing to initiate folding N protein + den. H20H20 denatured state D native state N single-exponential relaxa- tion for 2-state process: time (ms) 0100 200 300 spectroscopic signal
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Mutational analysis of 2-state folding G D T N Transition state theory: k exp(-G T–D ) D T N N’ T’ G Mutations change the folding rate k and stability G N–D Central quantities: -values G T–D G N–D
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= 1: mutated residue is native-like structured in T Traditional interpretation of D T N N’ T’ G G = 0: mutated residue is unstructured in T D T N N’ T’
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: degree of structure formation of a residue in T Inconsistencies: - some ’s are 1 - different mutations of the same residue can have different -values -values Goldenberg, NSB 1999 Traditional interpretation of
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Example: -helix of CI2 S12G S12A E15D E15N A16G K17G K18G I20V L21A L21G D23A K24G 0.29 0.43 0.22 0.53 1.06 0.38 0.70 0.40 0.25 0.35 -0.25 0.10 mutation Itzhaki, Otzen, Fersht,1995 -values for mutations in the helix range from -0.25 to 1.06 Our finding:
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Mutational -value analysis of the folding kinetics Modeling -values for -helices Modeling -values for small -sheet proteins
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Helix cooperativity we assume that a helix is either fully formed or not formed in transition- state conformation T i we have two structural parameters per helix: - the degree of secondary structure in T - the degree of tertiary structure t in T
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we split up mutation-induced free energy changes into secondary and tertiary components: general form of -values for mutations in an -helix: Splitting up free energies G D T N
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-values for -helix of CI2 general formula: 1.0 t 0.15 mutational data for CI2 helix: D23A
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-values for helix 2 of protein A general formula: mutational data for helix 2: 1.0 t 0.45 11 33 22
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Summary C Merlo, KA Dill, TR Weikl, PNAS 2005 TR Weikl, KA Dill, JMB 2007 Consistent interpretation of -values for helices: with two structural parameters: the degrees of secondary and tertiary structure formation in T by splitting up mutation-induced free energy changes into secondary and tertiary components
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Mutational -value analysis of the folding kinetics Modeling -values for -helices Modeling -values for small -sheet proteins
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Modeling 3-stranded -proteins WW domains are 3-stranded -proteins with two -hairpins we assume that each hairpin is fully formed or not formed in the transition state
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Evidence for hairpin cooperativity 3s is a designed 3-stranded -protein with 20 residues transition state rigorously determined from folding- unfolding MD simulations result: either hairpin 1 or hairpin 2 structured in T Rao, Settanni, Guarnera, Caflisch, JCP 2005
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A simple model for WW domains we have two transition- state conformations with a single hairpin formed -values have the general form: the folding rate is:
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-values for FBP WW domain a first test: ’s for mutations affecting only hairpin 1 should have value 1 general formula: exp
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theo exp single-parameter fit: 1 0.77 2 = 1- 1 0.23 -values for FBP WW domain general formula:
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Summary C Merlo, KA Dill, TR Weikl, PNAS 2005 TR Weikl, KA Dill, J Mol Biol 2007 TR Weikl, Biophys J 2008 Reconstruction of transition states from mutational -values based on: substructural cooperativity of helices and hairpins splitting up mutation-induced free energy changes
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