transition states in protein folding thomas weikl max planck institute of colloids and interfaces...

23
Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

Upload: lionel-bell

Post on 04-Jan-2016

218 views

Category:

Documents


3 download

TRANSCRIPT

Page 1: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

Transition States in Protein Folding

Thomas Weikl

Max Planck Institute of Colloids and InterfacesDepartment of Theory and Bio-Systems

Page 2: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

• Mutational -value analysis of the folding kinetics

• Modeling -values for -helices

• Modeling -values for small -sheet proteins

Overview

Page 3: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

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?

Page 4: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

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)

Page 5: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

2-state folding: Single molecules

• Donor and acceptor dyes at chain ends

Schuler et al., Nature 2002

• State-dependent transfer efficiency

Page 6: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

2-state folding: Protein ensemble

• rapid mixing to initiate foldingN

protein + den.

H20

denatured state D

native state N

• single-exponential relaxa-tion for 2-state process:

time (ms)0 100 200 300

spec

tros

copi

c si

gnal

Page 7: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

Mutational analysis of 2-state folding

G

D

T

N

• Transition state theory:

k exp(-GT–D)

D

T

N

N’

T’G

• Mutations change the folding

rate k and stability GN–D

• Central quantities: -values

GT–D

GN–D

Page 8: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

= 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’

Page 9: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

• : degree of structure formation of a residue in T

• Inconsistencies:

- some ’s are < 0 or > 1

- different mutations of

the same residue can

have different -values

-values

G

old

en

be

rg,

NS

B 1

99

9

Traditional interpretation of

Page 10: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

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:

Gα ΔGN

Page 11: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

• Mutational -value analysis of the folding kinetics

• Modeling -values for -helices

• Modeling -values for small -sheet proteins

Page 12: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

Helix cooperativity

• we assume that a helix is

either fully formed or

not formed in transition-

state conformation Ti

• we have two structural parameters per helix:

- the degree of secondary structure in T

- the degree of tertiary structure t in T

Page 13: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

• we split up mutation-induced free energy changes

into secondary and tertiary components:

• general form of -values for mutations in an -helix:

≡GT

ΔGN

= χ t + χ α − χ t( )ΔGα

ΔGN

Splitting up free energies

GT = χ α ΔGα + χ tΔGt

GN = ΔGα + ΔGt G

D

T

N

Page 14: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

-values for -helix of CI2

general formula:

=t + χα − χt( )ΔGα

ΔGN

1.0t 0.15

mutational data for CI2 helix:

Gα ΔGN

D23A

Page 15: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

-values for helix 2 of protein A

general formula:

=t + χα − χt( )ΔGα

ΔGN

mutational data for helix 2:

1.0t 0.45

1

3

2

Gα ΔGN

Page 16: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

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

Page 17: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

• Mutational -value analysis of the folding kinetics

• Modeling -values for -helices

• Modeling -values for small -sheet proteins

Page 18: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

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

Page 19: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

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

QuickTime™ and a decompressor

are needed to see this picture.

QuickTime™ and a decompressor

are needed to see this picture.

Page 20: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

A simple model for WW domains

• we have two transition-state conformations with a single hairpin formed

≡−RT Δlogk

ΔGN

=χ1ΔG1 + χ 2ΔG2

ΔGN

• -values have the general form:

• the folding rate is:

k ≈ 12 e −G1 R T + e −G 2 R T( )

Page 21: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

-values for FBP WW domain

• a first test: ’s for mutations affecting only hairpin 1 should have value 1

• general formula:

theo =χ 1ΔG1 + χ2ΔG2

ΔGN

exp

Page 22: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

theo

exp

• single-parameter fit:

1 0.772 = 1- 1 0.23

-values for FBP WW domain

• general formula:

theo =χ 1ΔG1 + χ2ΔG2

ΔGN

Page 23: Transition States in Protein Folding Thomas Weikl Max Planck Institute of Colloids and Interfaces Department of Theory and Bio-Systems

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