Phi-analysis of the folding of the B domain of protein A using multiple optical probes

We examined the co-operativity of ultra-fast folding of a protein and whether the Phi-value analysis of its transition state depended on the location of the optical probe. We incorporated in turn a tryptophan residue into each of the three helices of the B domain of Protein A. Each Trp mutant of the three-helix bundle protein was used as a pseudo-wild-type parent for Phi-analysis in which the intrinsic Trp fluorescence probed the formation of each helix during the transition state. Apart from local effects in the immediate vicinity of the probe, the three separate sets of Phi-values were in excellent agreement, demonstrating the overall co-operativity of folding and the robustness of the Phi-analysis. The transition state of folding of Protein A contains the second helix being well formed with many stabilizing tertiary hydrophobic interactions. In contrast, the first and the third helices are more poorly structured in the transition state. The mechanism of folding thus involves the concurrent formation of secondary and tertiary interactions, and is towards the nucleation-condensation extreme in the nucleation-condensation-framework continuum of mechanism, with helix 2 being the nucleus. We provide an error analysis of Phi-values derived purely from the kinetics of two-state chevron plots.     

Characterization of the folding kinetics of a three-helix bundle protein via a minimalist Langevin model.

We use a simple off-lattice Langevin model of protein folding to characterize the folding and unfolding of a fast-folding, 46 residue three-helix bundle. Under conditions at which the C-terminal helix is 30 % stable, we observe a clear three-state folding mechanism. In the on-pathway intermediate state, the middle and C-terminal helices are folded and in contact with each other, while the N-terminal region remains disordered. Nevertheless, under these conditions this intermediate is thermodynamically unstable relative to its unfolded state. The first and highest folding barrier corresponds to the organization of the hinge between the middle and C-terminal helices. A subsequent major barrier corresponds to the organization of the hinge between the middle and N-terminal helices. Hyperstabilizing the hinge regions leads to twice the folding rate that is obtained from hyperstabilizing the helices, even though much fewer contacts are involved in hinge hyperstabilization than in helix hyperstabilization. Unfolding follows single-exponential kinetics, even at temperatures only slightly above the folding transition temperature.     

Diffusing and colliding: the atomic level folding/unfolding pathway of a small helical protein

Proteins with ultra-fast folding/unfolding kinetics are excellent candidates for study by molecular dynamics. Here, we describe such simulations of a three helix bundle protein, the engrailed homeodomain (En-HD), which folds via the diffusion-collision model. The unfolding pathway of En-HD was characterized by seven simulations of the protein and 12 simulations of its helical fragments yielding over 1.1 micros of simulation time in water. Various conformational states along the unfolding pathway were identified. There is the compact native-like transition state, a U-shaped helical intermediate and an unfolded state with dynamic helical segments. Each of these states is in good agreement with experimental data. Examining these states as well as the transitions between them, we find the role of long-range tertiary contacts, specifically salt-bridges, important in the folding/unfolding pathway. In the folding direction, charged residues form long-range tertiary contacts before the hydrophobic core is formed. The formation of HII is assisted by a specific salt-bridge and by non-specific (fluctuating) tertiary contacts, which we call contact-assisted helix formation. Salt-bridges persist as the protein approaches the transition state, stabilizing HII until the hydrophobic core is formed. To complement this information, simulations of fragments of En-HD illustrate the helical propensities of the individual segments. By thermal denaturation, HII proved to be the least stable helix, unfolding in less than 450 ps at high temperature. We observed the low helical propensity of C-terminal residues from HIII in fragment simulations which, when compared to En-HD unfolding simulations, link the unraveling of HIII to the initial event that drives the unfolding of En-HD.     

Importance of context in protein folding: secondary structural propensities versus tertiary contact-assisted secondary structure formation

Molecular dynamics simulations can be used to reveal the detailed conformational behaviors of peptides and proteins. By comparing fragment and full-length protein simulations, we can investigate the role of each peptide segment in the folding process. Here, we take advantage of information regarding the helix formation process from our previous simulations of barnase and protein A as well as new simulations of four helical fragments from these proteins at three different temperatures, starting with both helical and extended structures. Segments with high helical propensity began the folding process by tethering the chain through side chain interactions involving either polar interactions, such as salt bridges, or hydrophobic staples. These tethers were frequently nonnative (i.e., not i --> i + 4 spacing) and provided a scaffold for other residues, thereby limiting the conformational search. The helical structure then propagated on both sides of the tether. Segments with low stability and propensity formed later in the folding process and utilized contacts with other portions of the protein when folding. These helices formed via a tertiary contact-assisted mechanism, primarily via hydrophobic contacts between residues distant in sequence. Thus, segments with different helical propensities appear to play different roles during protein folding. Furthermore, the active role of nonlocal side chains in helix formation highlights why we must move beyond simple hierarchical models of protein folding.     

Identification of native and non-native structure in kinetic folding intermediates of apomyoglobin

Site-directed mutagenesis has been used to probe the interactions that stabilize the equilibrium and burst phase kinetic intermediates formed by apomyoglobin. Nine bulky hydrophobic residues in the A, E, G and H helices were replaced by alanine, and the effects on protein stability and kinetic folding pathways were determined. Hydrogen exchange pulse-labeling experiments, with NMR detection, were performed for all mutants. All of the alanine substitutions resulted in changes in proton occupancy or an increased rate of hydrogen-deuterium exchange for amides in the immediate vicinity of the mutation. In addition, most mutations affected residues in distant parts of the amino acid sequence, providing insights into the topology of the burst phase intermediate and the interactions that stabilize its structure. Differences between the pH 4 equilibrium molten globule and the kinetic intermediate are evident: the E helix region plays no discernible role in the equilibrium intermediate, but contributes significantly to stabilization of the ensemble of compact intermediates formed during kinetic refolding. Mutations that interfere with docking of the E helix onto the preformed A/B/G/H helix core substantially decrease the folding rate, indicating that docking and folding of the E helix region occurs prior to formation of the apomyoglobin folding transition state. The results of the mutagenesis experiments are consistent with rapid formation of an ensemble of compact burst phase intermediates with an overall native-like topological arrangement of the A, B, E, G, and H helices. However, the experiments also point to disorder in docking of the E helix and to non-native contacts in the kinetic intermediate. In particular, there is evidence for translocation of the H helix by approximately one helical turn towards its N terminus to maximize hydrophobic interactions with helix G. Thus, the burst phase intermediate observed during kinetic refolding of apomyoglobin consists of an ensemble of compact, kinetically trapped states in which the helix docking appears to be topologically correct, but in which there are local non-native interactions that must be resolved before the protein can fold to the native structure.     

Conformational and dynamic characterization of the molten globule state of an apomyoglobin mutant with an altered folding pathway.

Kinetic and equilibrium studies of apomyoglobin folding pathways and intermediates have provided important insights into the mechanism of protein folding. To investigate the role of intrinsic helical propensities in the apomyoglobin folding process, a mutant has been prepared in which Asn132 and Glu136 have been substituted with glycine to destabilize the H helix. The structure and dynamics of the equilibrium molten globule state formed at pH 4.1 have been examined using NMR spectroscopy. Deviations of backbone (13)C(alpha) and (13)CO chemical shifts from random coil values reveal high populations of helical structure in the A and G helix regions and in part of the B helix. However, the H helix is significantly destabilized compared to the wild-type molten globule. Heteronuclear [(1)H]-(15)N NOEs show that, although the polypeptide backbone in the H helix region is more flexible than in the wild-type protein, its motions are restricted by transient hydrophobic interactions with the molten globule core. Quench flow hydrogen exchange measurements reveal stable helical structure in the A and G helices and part of the B helix in the burst phase kinetic intermediate and confirm that the H helix is largely unstructured. Stabilization of structure in the H helix occurs during the slow folding phases, in synchrony with the C and E helices and the CD region. The kinetic and equilibrium molten globule intermediates formed by N132G/E136G are similar in structure. Although both the wild-type apomyoglobin and the mutant fold via compact helical intermediates, the structures of the intermediates and consequently the detailed folding pathways differ. Apomyoglobin is therefore capable of compensating for mutations by using alternative folding pathways within a common basic framework. Tertiary hydrophobic interactions appear to play an important role in the formation and stabilization of secondary structure in the H helix of the N132G/E136G mutant. These studies provide important insights into the interplay between secondary and tertiary structure formation in protein folding.     

The structure of the major transition state for folding of an FF domain from experiment and simulation

We have analysed the transition state of folding of the four-helix FF domain from HYPA/FBP11 by high-resolution experiment and simulation as part of a continuing effort to understand the principles of folding and the refinement of predictive methods. The major transition state for folding was subjected to a Phi-value analysis utilising 50 mutants. The transition state contained a nucleus for folding centred around the end of helix 1 (H1) and the beginning of helix 2 (H2). Secondary structure in this region was fully formed (PhiF=0.9-1) and tertiary interactions were well developed. Interactions in the distal part of the native structure were weak (PhiF=0-0.2). The hydrophobic core and other parts of the protein displayed intermediate Phi-values, suggesting that interactions coalesce as the end of H1 and beginning of H2 are in the process of being formed. The distribution of Phi-values resembled that of barnase, which folds via an intermediate, rather than that of CI2 which folds by a concerted nucleation-condensation mechanism. The overall picture of the transition state structure identified in molecular dynamics simulations is in qualitative agreement, with the turn connecting H1 and H2 being formed, a loosened core, and H4 partially unfolded and detached from the core. There are some differences in the details and interpretation of specific Phi-values.     

Proline residues in transmembrane alpha helices affect the folding of bacteriorhodopsin

Proline residues occur frequently in transmembrane alpha helices, which contrasts with their behaviour as helix-breakers in water-soluble proteins. The three membrane-embedded proline residues of bacteriorhodopsin have been replaced individually by alanine and glycine to give P50A, or P50G on helix B, P91A, or P91G on helix C, and P186A or P186G on helix F, and the effect on the protein folding kinetics has been investigated. The rate-limiting apoprotein folding step, which results in formation of a seven transmembrane, alpha helical state, was slower than wild-type protein for the Pro50 and Pro91 mutants, regardless of whether they were mutated to Ala or Gly. These proline residues give rise to several inter-helix contacts, which are therefore important in folding to the seven transmembrane helix state. No evidence for cis-trans isomerisations of the peptidyl prolyl bonds was found during this rate-limiting apoprotein folding step. Mutations of all three membrane-embedded proline residues affected the subsequent retinal binding and final folding to bacteriorhodopsin, suggesting that these proline residues contribute to formation of the retinal binding pocket within the helix bundle, again via helix/helix interactions. These results point to proline residues in transmembrane alpha helices being important in the folding of integral membrane proteins. The helix/helix interactions and hydrogen bonds that arise from the presence of proline residues in transmembrane alpha helices can affect the formation of transmembrane alpha helix bundles as well as cofactor binding pockets.     

Dynamic Monte Carlo simulations of globular protein folding/unfolding pathways. II. Alpha-helical motifs

Dynamic Monte Carlo simulations of the folding pathways of alpha-helical protein motifs have been undertaken in the context of a diamond lattice model of globular proteins. The first question addressed in the nature of the assembly process of an alpha-helical hairpin. While the hairpin could, in principle, be formed via the diffusion-collision-adhesion of isolated performed helices, this is not the dominant mechanism of assembly found in the simulations. Rather, the helices that form native hairpins are constructed on-site, with folding initiating at or near the turn in almost all cases. Next, the folding/unfolding pathways of four-helix bundles having tight bends and one and two long loops in the native state are explored. Once again, an on-site construction mechanism of folding obtains, with a hairpin forming first, followed by the formation of a three-helix bundle, and finally the fourth helix of the native bundle assembles. Unfolding is essentially the reverse of folding. A simplified analytic theory is developed that reproduces the equilibrium folding transitions obtained from the simulations remarkably well and, for the dominant folding pathway, correctly identifies the intermediates seen in the simulations. The analytic theory provides the free energy along the reaction co-ordinate and identifies the transition state for all three motifs as being quite close to the native state, with three of the four helices assembled, and approximately one turn of the fourth helix in place. The transition state is separated from the native conformation by a free-energy barrier of mainly energetic origin and from the denatured state by a barrier of mainly entropic origin. The general features of the folding pathway seen in all variants of the model four-helix bundles are similar to those observed in the folding of beta-barrel, Greek key proteins; this suggests that many of the qualitative aspects of folding are invariant to the particular native state topology and secondary structure.     

Conservation of folding pathways in evolutionarily distant globin sequences

To test the hypothesis that the folding pathways of evolutionarily related proteins with similar three-dimensional structures but widely different sequences should be similar, the folding pathway of apoleghemoglobin has been characterized using stopped-flow circular dichroism, heteronuclear NMR pulse labeling techniques and mass spectrometry. The pathway of folding was found to differ significantly from that of a protein of the same family, apomyoglobin, although both proteins appear to fold through helical burst phase intermediates. For leghemoglobin, the burst phase intermediate exhibits stable helical structure in the G and H helices, together with a small region in the center of the E helix. The A and B helices are not stabilized until later stages of the folding process. The structure of the burst phase folding intermediate thus differs from that of apomyoglobin, in which stable helical structure is formed in the A, B, G and H helix regions.     

Characterisation of the conformational properties of urea-unfolded Im7: implications for the early stages of protein folding

The colicin immunity protein Im7 folds from its unfolded state in 6 M urea to its native four-helix structure through an on-pathway intermediate that lacks one of the helices of the native structure (helix III). In order to further characterize the folding mechanism of Im7, we have studied the conformational properties of the protein unfolded in 6 M urea in detail using heteronuclear NMR. Triple-resonance experiments with 13C/15N-labelled Im7 in 6 M urea provided almost complete resonance assignments for the backbone nuclei, and measurement of backbone 15N relaxation parameters allowed dynamic ordering of the unfolded polypeptide chain to be investigated. Reduced spectral density mapping and fitting backbone R2 relaxation rates to a polymer dynamics model identified four clusters of interacting residues, each predicted by the average area buried upon folding for each residue. Chemical shift analyses and measurement of NOEs detected with a long mixing-time 1H-1H-15N NOESY-HSQC spectrum confirmed the formation of four clusters. Each cluster of interacting side-chains in urea-unfolded Im7 occurs in a region of the protein that forms a helix in the protein, with the largest clusters being associated with the three long helices that are formed in the on-pathway folding intermediate, whilst the smallest cluster forms a helix only in the native state. NMR studies of a Phe15Ala Im7 variant and a protein in which residues 51-56 are replaced by three glycine residues (H3G3 Im7*), indicated that the clusters do not interact with each other, possibly because they are solvated by urea, as indicated by analysis of NOEs between the protein and the solvent. Based on these data, we suggest that dilution of the chaotrope to initiate refolding will result in collapse of the clusters, leading to the formation of persistent helical structure and the generation of the three-helix folding intermediate.     

Sequence-based study of two related proteins with different folding behaviors

Z(SPA-1) is an engineered protein that binds to its parent, the three-helix-bundle Z domain of staphylococcal protein A. Uncomplexed Z(SPA-1) shows a reduced helix content and a melting behavior that is less cooperative, compared with the wild-type Z domain. Here we show that the difference in folding behavior between these two sequences can be partly understood in terms of an off-lattice model with 5-6 atoms per amino acid and a minimalistic potential, in which folding is driven by backbone hydrogen bonding and effective hydrophobic attraction.     

Im7 folding mechanism: misfolding on a path to the native state

Many proteins populate collapsed intermediate states during folding. In order to elucidate the nature and importance of these species, we have mapped the structure of the on-pathway intermediate of the four-helix protein, Im7, together with the conformational changes it undergoes as it folds to the native state. Kinetic data for 29 Im7 point mutants show that the intermediate contains three of the four helices found in the native structure, packed around a specific hydrophobic core. However, the intermediate contains many non-native interactions; as a result, hydrophobic interactions become disrupted in the rate-limiting transition state before the final helix docks onto the developing structure. The results of this study support a hierarchical mechanism of protein folding and explain why the misfolding of Im7 occurs. The data also demonstrate that non-native interactions can play a significant role in folding, even for small proteins with simple topologies.     

Critical role of beta-hairpin formation in protein G folding

Comparison of the folding mechanisms of proteins with similar structures but very different sequences can provide fundamental insights into the determinants of protein folding mechanisms. Despite very little sequence similarity, the approximately 60 residue IgG binding domains of protein G and protein L both consist of a single helix packed against a four-stranded sheet formed by two symmetrically disposed beta-hairpins. We demonstrate that, as in the case of protein L, one of the two beta-turns of protein G is formed and the other disrupted in the folding transition state. Unlike protein L, however, in protein G it is the second beta-turn that is formed in the folding transition state ensemble. Substitution of an Asp residue by Ala in protein G that eliminates an i,i+2 side chain-main chain hydrogen bond in the second beta-turn slows the folding rate approximately 20-fold but has virtually no effect on the unfolding rate. Taken together with previous results, these findings suggest that the presence of an intact beta-turn in the folding transition state is a consequence of the overall topology of protein L and protein G, but the particular hairpin that is formed is determined by the detailed interatomic interactions that determine the free energies of formation of the isolated beta-hairpins.     

Trapping the on-pathway folding intermediate of Im7 at equilibrium

The four-helical protein Im7 folds via a rapidly formed on-pathway intermediate (k(UI)=3000 s(-1) at pH 7.0, 10 degrees C) that contains three (helices I, II and IV) of the four native alpha-helices. The relatively slow (k(IN)=300 s(-1)) conversion of this intermediate into the native structure is driven by the folding and docking of the six residue helix III onto the developing hydrophobic core. Here, we describe the structural properties of four Im7* variants designed to trap the protein in the intermediate state by disrupting the stabilising interactions formed between helix III and the rest of the protein structure. In two of these variants (I54A and L53AI54A), hydrophobic residues within helix III have been mutated to alanine, whilst in the other two mutants the sequence encompassing the native helix III was replaced by a glycine linker, three (H3G3) or six (H3G6) residues in length. All four variants were shown to be monomeric, as judged by analytical ultracentrifugation, and highly helical as measured by far-UV CD. In addition, all the variants denature co-operatively and have a stability (DeltaG(UF)) and buried hydrophobic surface area (M(UF)) similar to those of the on-pathway kinetic intermediate. Structural characterisation of these variants using 1-anilino-8-napthalene sulphonic acid (ANS) binding, near-UV CD and 1D (1)H NMR demonstrate further that the trapped intermediate ensemble is highly structured with little exposed hydrophobic surface area. Interestingly, however, the structural properties of the variants I54A and L53AI54A differ in detail from those of H3G3 and H3G6. In particular, the single tryptophan residue, located near the end of helix IV, and distant from helix III, is in a distinct environment in the two sets of mutants as judged by fluorescence, near-UV CD and the sensitivity of tryptophan fluorescence to iodide quenching. Overall, the results confirm previous kinetic analysis that demonstrated the hierarchical folding of Im7 via an on-pathway intermediate, and show that this species is a highly helical ensemble with a well-formed hydrophobic core. By contrast with the native state, however, the intermediate ensemble is flexible enough to change in response to mutation, its structural properties being tailored by residues in the sequence encompassing the native helix III.     

Protein folding: matching theory and experiment.

The impact of folding funnels and folding simulations on the way experimentalists interpret results is examined. The image of the transition state has changed from a unique species that has a strained configuration, with a correspondingly high free energy, to a more ordinary folding intermediate, whose balance between limited conformational entropy and stabilizing contacts places it at the top of the free energy barrier. Evidence for a broad transition barrier comes from studies showing that mutations can change the position of the barrier. The main controversial issue now is whether populated folding intermediates are productive on-pathway intermediates or dead-end traps. Direct experimental evidence is needed. Theories suggesting that populated intermediates are trapped in a glasslike state are usually based on mechanisms which imply that trapping would only be extremely short-lived (e.g., nanoseconds) in water at 25 degrees C. There seems to be little experimental evidence for long-lived trapping in monomers, if folding aggregates are excluded. On the other hand, there is good evidence for kinetic trapping in dimers. alpha-Helix formation is currently the fastest known process in protein folding, and incipient helices are present at the start of folding. Fast helix formation has the effect of narrowing drastically the choice of folding routes. Thus helix formation can direct folding. It changes the folding metaphor from pouring liquid down a folding funnel to a train leaving a switchyard with only a few choices of exit tracks.     

Characterization of the unfolding pathway of the cell-cycle protein p13suc1 by molecular dynamics simulations: implications for domain swapping

BACKGROUND: The p13suc1 gene product is a member of the cks (cyclin-dependent protein kinase subunit) protein family and has been implicated in regulation of the cell cycle. Various crystal structures of suc1 are available, including a globular, monomeric form and a beta-strand exchanged dimer. It has been suggested that conversions between these forms, and perhaps others, may be important in the regulation of the cell cycle. RESULTS: We have undertaken molecular dynamics simulations of protein unfolding to investigate the conformational properties of suc1. Unfolding transition states were identified for each of four simulations. These states contain some native secondary structure, primarily helix alpha1 and the core of the beta sheet. The hydrophobic core is loosely packed. Further unfolding leads to an intermediate state that is slightly more expanded than the transition state, but with considerably fewer nonlocal, tertiary packing contacts and less secondary structure. The helices are fluctuating but partially formed in the denatured state and beta2 and beta4 remain associated. CONCLUSIONS: It appears that suc1 folds by a nucleation-condensation mechanism, similar to that observed for two-state folding proteins. However, suc1 forms an intermediate during unfolding and contains considerable residual structure in the denatured state. The stability of the beta2-beta4 residual structure is surprising, because beta4 is the strand involved in domain swapping. This stability suggests that the domain-swapping event, if physiologically relevant, may require the assistance of additional factors in vivo or occur early in the folding process.     

Amino Acid Insertion Reveals a Necessary Three-Helical Intermediate in the Folding Pathway of the Colicin E7 Immunity Protein Im7

The small (87-residue) α-helical protein Im7 (an inhibitor protein for colicin E7 that provides immunity to cells producing colicin E7) folds via a three-state mechanism involving an on-pathway intermediate. This kinetic intermediate contains three of four native helices that are oriented in a non-native manner so as to minimise exposed hydrophobic surface area at this point in folding. The short (6-residue) helix III has been shown to be unstructured in the intermediate ensemble and does not dock onto the developing hydrophobic core until after the rate-limiting transition state has been traversed. After helix III has docked, it adopts an α-helical secondary structure, and the side chains of residues within this region provide contacts that are crucial to native-state stability. In order to probe further the role of helix III in the folding mechanism of Im7, we created a variant that contains an eight-amino-acid polyalanine-like helix stabilised by a Glu-Arg salt bridge and an Asn-Pro-Gly capping motif, juxtaposed C-terminal to the natural 6-residue helix III. The effect of this insertion on the structure of the native protein and its folding mechanism were studied using NMR and ?-value analysis, respectively. The results reveal a robust native structure that is not perturbed by the presence of the extended helix III. Mutational analysis performed to probe the folding mechanism of the redesigned protein revealed a conserved mechanism involving the canonical three-helical intermediate. The results suggest that folding via a three-helical species stabilised by both native and non-native interactions is an essential feature of Im7 folding, independent of the helical propensity of helix III.     

Transition-states in protein folding kinetics: the structural interpretation of Phi values

Phi values are experimental measures of the effects of mutations on the folding kinetics of a protein. A central question is what structural information Phi values give about the transition-state of folding. Traditionally, a Phi value is interpreted as representing the "nativeness" of a mutated residue in the transition-state. However, this interpretation is often problematic. We present here a better structural interpretation of Phi values for mutations within a given helix. Our interpretation is based on a simple physical model that distinguishes between secondary and tertiary free energy contributions of helical residues. From a linear fit of the model to experimental data, we obtain two structural parameters: the extent of helix formation in the transition-state, and the nativeness of tertiary interactions in the transition-state. We apply the model to all proteins with well-characterized helices for which more than 10 Phi values are available: protein A, CI2, and protein L. The model is simple to apply to experimental data, captures nonclassical Phi values <0 or >1 in these helices, and explains how different mutations at a given site can lead to different Phi values.     

Towards a complete description of the structural and dynamic properties of the denatured state of barnase and the role of residual structure in folding

The detailed characterization of denatured proteins remains elusive due to their mobility and conformational heterogeneity. NMR studies are beginning to provide clues regarding residual structure in the denatured state but the resulting data are too sparse to be transformed into molecular models using conventional techniques. Molecular dynamics simulations can complement NMR by providing detailed structural information for components of the denatured ensemble. Here, we describe three independent 4 ns high-temperature molecular dynamics simulations of barnase in water. The simulated denatured state was conformationally heterogeneous with respect to the conformations populated both within a single simulation and between simulations. Nonetheless, there were some persistent interactions that occurred to varying degrees in all simulations and primarily involved the formation of fluid hydrophobic clusters with participating residues changing over time. The region of the beta(3-4) hairpin contained a particularly high degree of such side-chain interactions but it lacked beta-structure in two of the three denatured ensembles: beta(3-4) was the only portion of the beta-structure to contain significant residual structure in the denatured state. The two principal alpha-helices (alpha1 and alpha2) adopted dynamic helical structure. In addition, there were persistent contacts that pinched off core 2 from the body of the protein. The rest of the protein was unstructured, aside from transient and mostly local side-chain interactions. Overall, the simulated denatured state contains residual structure in the form of dynamic, fluctuating secondary structure in alpha1 and alpha2, as well as fluctuating tertiary contacts in the beta(3-4) region, and between alpha1 and beta(3-4), in agreement with previous NMR studies. Here, we also show that these regions containing residual structure display impaired mobility by both molecular dynamics and NMR relaxation experiments. The residual structure was important in decreasing the conformational states available to the chain and in repairing disrupted regions. For example, tertiary contacts between beta(3-4) and alpha1 assisted in the refolding of alpha1. This contact-assisted helix formation was confirmed in fragment simulations of beta(3-4) and alpha1 alone and complexed, and, as such, alpha1 and beta(3-4) appear to be folding initiation sites. The role of these sites in folding was investigated by working backwards and considering the simulation in reverse, noting that earlier time-points from the simulations provide models of the major intermediate and transition states in quantitative agreement with data from both unfolding and refolding experiments. Both beta(3-4) and alpha1 are dynamic in the denatured state but when they collide and make enough contacts, they provide a loose structural scaffold onto which further beta-strands pack. The beta-structure condenses about beta(3-4), while alpha1 aids in stabilizing beta(3-4) and maintaining its orientation. The resulting beta-structure is relatively planar and loose in the major intermediate. Further packing ensues, and as a result the beta-sheet twists, leading to the major transition state. The structure is still expanded and loops are not well formed at this point. Fine-tuning of the packing interactions and the final condensation of the structure then occurs to yield the native state.