entropic and enthalpic barriers in cooperative protein folding hue sun c han departments of...

Entropic and Enthalpic Barriers in Cooperative Protein

FoldingHue Sun CHAN

Departments of Biochemistry, and of Molecular Genetics University of Toronto, Ontario M5S 1A8 Canada

http://biochemistry.utoronto.ca/chan/bch.html

IMA, January 17, 2008

What do we know from experiments?

Cooperative Folding:

How does the calorimetric criterion work?

bimodal cooperative folding

unimodal noncooperative folding

Kinetic manifestation of folding cooperativity: linear chevron plots

Linear folding and unfolding arms imply a linear relationship between log(folding/unfolding rate) and equilibrium stability

Data from Jackson et al., Biochemistry 32:11270 (1993)

chevron rollover is indicative of less cooperative or noncooperative folding

Do we understand the

Physics of

Generic Protein Properties?

Most current coarse-grained protein chain models do not satisfy experimental cooperativity criteria

Chan et al., Methods Enzymol (2004)

Clementi et al., JMB (2000); Koga & Takada, JMB (2001); Kaya & Chan, JMB (2003)

Continuum C Go Models

Native-centric local and non-bonded interactions

Langevin dynamics

Thermodynamically quite cooperative

CI2

Go-model chevron plots have significant chevron rollovers, implying that in many cases Go models are less cooperative than the real proteins they aim to mimick

Jackson & Fersht, Biochemistry (1991)

Kaya & Chan, JMB (2003)

Theory

Experiment

Even with native biases, pairwise additive coarse-grained interactions do not account for cooperative folding

Better Mesoscopic Principles?

(local-nonlocal coupling) Kaya & Chan, Proteins

(2003)

‘Many-body’ interactions needed to account for folding cooperativity

A hypothesized cooperative interplay between favorable nonlocal interactions and local conformational preferences

Testing the local-nonlocal coupling idea by lattice models

a < 1, attentuation factor

Kaya & Chan, Proteins (2003)

Native Topology (Contact Pattern) Dependent Folding Rates

Plaxco, Simons & Baker, JMB (1998)

Plot from Plaxco et al. Biochemistry (2000)

Can protein chain models capture this trend?

Kaya & Chan, Proteins (2003); Chan et al., Methods Enzymol (2004)

Many-body interactions in the form of local-nonlocal coupling rationalize topology-dependent folding rates

Top7, 1qys (93aa) Kuhlman et al., Science (2003)

Scalley-Kim & Baker, JMB (2004); Watters et al., Cell (2007)


Our theoretical perspective was corroborated by experiments:

Cooperativity is likely an evolutionarily selected trait; cooperativity is not a corollary of a protein’s ability to fold

theory

experiment

Folding Barriers

entropic & enthalpic components

Entropic Barriers:

Role of conformational entropic barriers in native topology-dependent folding rates

Wallin & Chan, J Phys Condens Matt (2006)


Transition-state ensembles:

1div 1pg

b

1imq1wit

‘Transition state’ as conformations around the Q barrier

Q = fractional number

of native contacts

Wallin & Chan, J Phys Condens Matt (2006); cf. Koga & Takada, JMB (2001)

… found some correlation between model and experimental folding rates, suggesting that the model captures part of the physics


Entropic barriers:

The topology-folding rate relationship is likely dominated by conformational entropy effect

lower temperature

Enthalpic barriers:

non-Arrhenius folding rates, positive unfoled-to-transition state enthalpy changes at some temperatures

Does this mean that the folding landscape is not funnel-like?

H

S

Cp

Thermodynamic Signatures of Protein Folding Kinetics

CI2 “reaction profiles”

25 °C

25 °C

enthalpic barrier

Desolvation is a likely origin of robust enthalpic barriers to protein folding

Liu & Chan, JMB (2005)

Liu & Chan, JMB (2005); Phys Biol (2005); cf. Cheung et al., PNAS (2002); Kaya & Chan, JMB (2003)

Desolvation barriers enhance folding/unfolding cooperativity increasing

height of pairwise desolvation barrier leads to …

Higher overall free energy barrier

more linear chevron plots

CI2

CI2

less native fluctuation

A. Ferguson, Z. Liu & H.S. Chan (2007)

Desolvation barrier effects are a likely contributor to the remarkable diversity in the folding rates of small proteins

simulated folding rates span ~4.5 orders of magnitude

simulated folding rates span ~1.5 orders of magnitude

…but pairwise desolvation barriers alone are insufficient to account for the thermodynamic signatures of cooperative folding

Typically, Unfolded-to-Transition-State heat capacity change is negative for protein folding, but …

for the association of small nonpolar solutes in water, heat capacity change is positive around the desolvation free energy barrier.

Length-scale dependence provides a possible probe for cooperativity?

from G at 8 temperatures

Shimizu & Chan, JACS (2001)

TIP4P water model

CP highly non-monotonic

Not well predicted by surface areas

rnm

r

CH4

Xe

3-body

2-body

Paschek, J Chem Phys 120:6674 (2004)Moghaddam, Shimizu & Chan, JACS (2005)

Hydrophobic interactions among small hydrophobic solutes:

Robust CP > 0 at the desolvation free energy barrier

Moghaddam, Shimizu & Chan, JACS (2005); Liu & Chan, JMB (2005)

Enthalpic barrier can be significantly higher than the desolvation free energy barrier

temperature dependence of the potential of mean force (PMF)

Enthalpy-Entropy Compensation at Desolvation

MacCallum, Moghaddam, Chan & Tieleman, PNAS (2007)

Helix association in water as a model for rate-limiting events in protein folding A pair of 20-

residue

poly-alanine or

poly-leucine helices

~3,800 water molecules

Simulated constant-pressure free energy of association (potential of mean force, PMF) at five temperatures


Enthalpic desolvation barriers of ~ 50 kJ/mol comparable to that of protein foldingDramatic enthalpy-entropy compensation at the desolvation step leading to low or non-existent free energy barriers

At 25 deg C,

Enthalpic folding barrier height for

CI2 is ~ 30kJ/mol (Oliveberg et al., 1995)

CspB is ~ 32kJ/mol (Schindler & Schmid, 1996)


Enthalpic barriers caused by steric dewetting

Recap.:Folding cooperativity implies ‘near-Levinthal’ funnels

Enthalpic barriers can be consistent with funnel-like folding landscapes

?

Artem Badasyan

Allison Ferguson

Mikael Borg

Huseyin Kaya

Michael Knott

Zhirong Liu

Maria Sabaye Moghaddam

Seishi Shimizu

Stefan Wallin

Co-workers

University of Toronto University of Toronto

Prof. D. Peter Tieleman

Justin MacCallumUniversity of MuensterProf. Erich Bornberg-Bauer

David Vernazobres

Richard Wroe

University of Calgary

Prof. Julie D. Forman-KayProf. Regis Pomes

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