Title: Folding
1Folding
- Anfinsen
- cooperativity
- time scales, speed range
- Levinthal paradox
- ensembles
- energy landscape funnel
- chaperones
- thermodynamics, 15 kcal/mol
- denaturation thermal, chemical
- 2-state vs. intermediates, phi-values
- contact order as a metric of "foldedness"
- lattice models (Shakhnovich, Dill, Skolnick)
2Folding
- Anfinsen (1950s) showed reversibility of
denaturation with urea for RNase A - amino acid sequence encodes struct thermodynamic
hypothesis - exception is chaperones (also role of disulfides,
Pro isomerization) - folding is cooperative
differential scanning calorimetry
3Time-scales for folding
- cytochrome b562 5 ms
- lambda repressor 0.67 ms
- rat IFABP 33 ms
- CRABP 1 24.5 sec
- tryptophan synthase b2-subunit 992 sec (396 aa)
4Kubelka et al (2004)
5Galzitskaya et al. (2003)
6Folding, Unfolding, and Re-folding
- at equilibrium, proteins represent an ensemble,
with some unfolded (constantly unfolding and
refolding) - thermodynamic ensembles (Boltzmann distribution)
- can measure with hydrogen-exchange (NMR)
- even buried Hs exchange with solvent at some
rate - reflects dynamic unfolding/refolding
- overall folding rate const vs. kunfold and kfold
- equilibrium shifted in direction of DG
7Thermodynamic vs. kinetic control?
- do folded structures represent true global energy
minimum, or just kinetically accessible local
minima? - what causes slow folding a high transition-state
barrier, or just a large space to search?
8Levinthal Paradox
- How can proteins fold in such a short time?
- Number of degrees of freedom
- gt2Nres (phi/psi angles), lt310Nres (atomic
coords) - states 3N3N? (backbone a/b/coil side-chain
rotamers) - how can this large space possibly be sampled to
find the global minimum? - intermediates and cooperativity
- collapse of hydrophobic core
- formation of key secondary structures
- folding pathway
- off-pathway intermediates (local minima) can act
as traps and slow-down the folding process
9- energy landscape funnel
- new view not just one preferred path
- many routes lead to min
- hydrogen-exchange
- natural/fast folding sequence have minimally
frustrated energy landscapes
10Two-state folding
- data must fit first-order kinetics
- linearity of ln(kf) vs. denaturant
- DG is same whether determined by kinetic vs.
thermodynamic (equilibrium) methods - no intermediates (at least not well-defined)
- what does the (transient) transition state look
like? - molten globule (Ptitsyn) collapsed but not
tightly-packed, rapidly fluctuating - stopped-flow hydrogen-exchange shows
native-like secondary structure signatures
(BPTI, a-lactalbumin) - bT measure of where transition occurs along
reaction coordinate how native-like?
11- Jackson and Fersht (1991) chymotrypsin
inhibitor 2
1. 2-state model supported by concordance of
params between thermo. and kinetics 2. slope (mF
and mU) correlates with difference in
accessible surface area between U and F (Myers,
Pace, and Scholtz, 1995) 3. if Kuku/kf and
kukuH20mfGCl and kfkfH2O-muGCl, then
mmumf
3-state barnase
rates!
re-folding (stopped flow)
unfolding (fluorescence curve)
equilibrium!
12van 't Hoff equation
Gibbs-Helmholtz equation
- Pace and Laurents (1989)
- Method for determining DCp
- - calorimeter (10 error)
- DCpd(DH)/dT from vHoff
- extrapolate from DG
- measured at different
- denaturant concentrations
balance between DS and DH
13Folding Pathway Intermediates
- hard to trap (low populated)
- non-linearity in chevrons in plots
- due to switch of dominant transition state
- intermediate CD spectra, hydrodynamic radius
- barnase (Fersht, 2000, PNAS)
- Sanchez and Keifhaber (2003) multiple examples
(conditions) - spectrin (Scott and Clarke, 2005)
broad transition vs. sequential intermediate
states?
14Lysozyme has both a fast a slow pathway
(Keifhaber, 1995) data fit better by a
double-exponential (t150ms, t2420ms)
see also Jamin and Baldwin (1996). folding vs.
unfolding rates as evidence for intermediates in
apomyoglobin
15- Valerie Daggett
- molecular dynamics simulation of
folding/unfolding - identification of order of sub-structure formation
simulations of ubiquitin at 498 K and 298 K
16Off-pathway intermediates
- BPTI 3 native disulfide bridges, 14-38, 30-51,
and 5-55 - other non-native bridges are formed during
folding in an oxidizing environment - proper folding follows specific order of
formation - making non-native disulfides forms kinetic
traps - can block free thiols and analyze population
distribution suggests thermodymamically
determined (equilibrium?)
show picture of interconversion of
intermediates...
17The Unfolded State
- random coil? (hydrodynamic radius)
- backbone, side-chains fully solvated (hydration)
- effects of pH, urea...
18Contact Order
- (Plaxco Simons Baker, 1998)
L length of protein N num of contact pairs
(side-chain dist lt 6A) DS sequence separation
1HRC, CO11.2
1UBQ, CO15.1
1TEN, CO17.4
19F-values
- Fersht AR, Matouschek A, Serrano L. (1992)
- a way of studying kinetics and folding
intermediates via mutation - if you mutate a residue that is a critical
(folded) part of an intermediate structure, you
might destabilize it, increasing the barrier, and
decreasing the rate of folding - if intermediate is structured and resembles
native, then mutation will affect stability of
each equally - it intermediate is unfolded, mutation will not
affect stability of TS - examples
- Crespo, Simpson, and Searle (2006) ubiquitin
- Bulaj Goldenberg (2001) - BPTI
phi0 no effect on TS
phi1 mutation affects TS
20Lattice Models
- Sali, Shakhnovich, and Karplus (1994)
- Monte Carlo sampling of configurations
- simplified interactions native contact1, else 0
- modeling secondary structure
- energy function sum over all contacts
- moves swap to neighboring site, avoid
self-intersection - Metropolis criterion accept if DElt0 or with
pgtexp(-DE/kT) - study which factors determine whether a random
sequence will fold (fast) - short-range vs. long-range contacts (contact
order)? - size? secondary structure? hydrophobicity?
- presence of a clearly-defined (deep) energy
minimum
21order parameter for heterogeneity of ensemble
(related to entropy)
synthetic example of a compact folded polymer
ends
cant move
22(No Transcript)
23- extensions
- Dill, HP model H and P atom types, 2D lattice
- off-lattice models
24Kolinski, Godzik, Skolnick (1993)
- ab initio folding?
- Cas only, on-lattice model (1.7Å spacing)
- side-chains modeled as spheres
- statistical side-chain contact potential (eij)
- non-directional H-bonds
- 4-body side-chain interactions
- cooperative coupling
25SICHO (Kolinski and Skolnick, 1998)
- ab initio folding with a few (20) restraints
(e.g. NMR) - model side-chains centers only (no Cas)
on-lattice - Monte Carlo moves multiple groups of atoms
- energy function simplified geometry statistics,
contact potentials
26Reduced-atom models
- Go (1980) model (off-lattice)
- Cas beads on a string (bond dist/angle
contraints) - good description in Hoang and Cieplak (2000).
- energy function includes term for native contacts
(springs) - application to mechanical unfolding of titin
27Mis-folding and Amyloid formation
- aggregation vs. fibril formation
- disease processes (20, Alzheimers, a-b)
- DLS dynamic light scattering
- solid-state crystallography
- kinetics (polymerization)
- similarity between 2 global minima
- dual-basin mis-folded intermediate for GFP
- Andrews et al (2008)
- http//www.pnas.org/ content/105/34/12283
Dobson (1998)