Coiled coils at the edge of configurational heterogeneity. Structural analyses of parallel and antiparallel homotetrameric coiled coils reveal configurational sensitivity to a single solvent-exposed amino acid substitution

A detailed understanding of the mechanisms by which particular amino acid sequences can give rise to more than one folded structure, such as for proteins that undergo large conformational changes or misfolding, is a long-standing objective of protein chemistry. Here, we describe the crystal structures of a single coiled-coil peptide in distinct parallel and antiparallel tetrameric configurations and further describe the parallel or antiparallel crystal structures of several related peptide sequences; the antiparallel tetrameric assemblies represent the first crystal structures of GCN4-derived peptides exhibiting such a configuration. Intriguingly, substitution of a single solvent-exposed residue enabled the parallel coiled-coil tetramer GCN4-pLI to populate the antiparallel configuration, suggesting that the two configurations are close enough in energy for subtle sequence changes to have important structural consequences. We present a structural analysis of the small changes to the helix register and side-chain conformations that accommodate the two configurations and have supplemented these results using solution studies and a molecular dynamics energetic analysis using a replica exchange methodology. Considering the previous examples of structural nonspecificity in coiled-coil peptides, the findings reported here not only emphasize the predisposition of the coiled-coil motif to adopt multiple configurations but also call attention to the associated risk that observed crytstal structures may not represent the only (or even the major) species present in solution.     

Restraint-driven formation of alpha-helical coiled coils in molecular dynamics simulations.

The alpha-helical coiled coil motif is among the first characterized and widely found architecture of protein structures. We report here a fast and reliable approach of simulated annealing molecular dynamics (SA/MD) for predicting the three-dimensional structures of various alpha-helical coiled coils of heptad repeat. One key element of our simulation involves a geometric restraint requiring residues occupying the first and fourth positions of the heptad to orient to the angle of their respective statistical average derived from a survey of coiled-coil structures deposited in the Protein Data Bank. Another is the incorporation of subunit rotation and inversion operations for generating symmetrized protein assemblies during the dynamics simulations. The procedure is fully automated and can be applied to different oligomerization states of identical subunits, as well as both parallel and antiparallel arrangements. Despite simplicity, the formation of five coiled-coil prototype systems driven by the restraint-based SA/MD approach shows that the level of prediction accuracy achieved previously by more elaborate procedures can be retained. The present work thus provides validation of a simulation approach that can be employed to utilize a wide variety of knowledge-based geometric restraints for structural prediction of symmetrical or pseudo-symmetrical protein systems.     

Importance of potential interhelical salt-bridges involving interior residues for coiled-coil stability and quaternary structure

Coiled coils are formed by two or more alpha-helices that align in a parallel or an antiparallel relative orientation. Polar interactions involving residues at the interior a and d positions are important for determining the quaternary structure of coiled coils. In the model heterodimeric coiled-coil Acid-a1-Base-a1, a buried a-d' Asn-Asn interaction is sufficient to specify both a dimeric structure and an antiparallel relative helix orientation. Although the equivalent a-a' interaction is found in parallel coiled coils, there is no example of an a-d' Asn-Asn interaction in structurally characterized, naturally occurring antiparallel coiled coils. Instead, interior charged residues form interhelical salt-bridges with residues at the adjacent e or g positions. Using a model coiled-coil heterodimer, we have explored the role of a potential interhelical interaction between an Arg at an interior d position and a Glu at the adjacent g' position. Our results demonstrate that this potentially attractive interhelical Coulombic interaction has little or no influence on helix orientation. Instead, we show that burying a single Arg residue at an interior position is sufficient to specify a dimeric state at a significantly lower thermodynamic cost than burial of two interacting Asn residues.     

A repeated coiled-coil interruption in the Escherichia coli condensin MukB

MukB, a divergent structural maintenance of chromosomes (SMC) protein, is important for chromosome segregation and condensation in Escherichia coli and other γ-proteobacteria. MukB and canonical SMC proteins share a common five-domain structure in which globular N- and C-terminal regions combine to form an ATP-binding-cassette-like ATPase domain. This ATPase domain is connected to a central, globular dimerization domain by a long antiparallel coiled coil. The structures of both globular domains have been solved recently. In contrast, little is known about the coiled coil, in spite of its clear importance for SMC function.Recently, we identified interacting regions on the N- and C-terminal halves of the MukB coiled coil through photoaffinity cross-linking experiments. On the basis of these low-resolution experimental constraints, phylogenetic data, and coiled-coil prediction analysis, we proposed a preliminary model in which the MukB coiled coil is divided into multiple segments. Here, we use a disulfide cross-linking assay to detect paired residues on opposite strands of MukB's coiled coil. This method provides accurate register data and demonstrates the presence of at least five coiled-coil segments in this domain. Moreover, these studies show that the segments are interrupted by a repeated, unprecedented deviation from canonical coiled-coil structure. These experiments provide a sufficiently detailed view of the MukB coiled coil to allow rational manipulation of this region for the first time, opening the door for structure-function studies of this domain.     

Predicting helix orientation for coiled-coil dimers

The alpha-helical coiled coil is a structurally simple protein oligomerization or interaction motif consisting of two or more alpha helices twisted into a supercoiled bundle. Coiled coils can differ in their stoichiometry, helix orientation, and axial alignment. Because of the near degeneracy of many of these variants, coiled coils pose a challenge to fold recognition methods for structure prediction. Whereas distinctions between some protein folds can be discriminated on the basis of hydrophobic/polar patterning or secondary structure propensities, the sequence differences that encode important details of coiled-coil structure can be subtle. This is emblematic of a larger problem in the field of protein structure and interaction prediction: that of establishing specificity between closely similar structures. We tested the behavior of different computational models on the problem of recognizing the correct orientation--parallel vs. antiparallel--of pairs of alpha helices that can form a dimeric coiled coil. For each of 131 examples of known structure, we constructed a large number of both parallel and antiparallel structural models and used these to assess the ability of five energy functions to recognize the correct fold. We also developed and tested three sequence-based approaches that make use of varying degrees of implicit structural information. The best structural methods performed similarly to the best sequence methods, correctly categorizing approximately 81% of dimers. Steric compatibility with the fold was important for some coiled coils we investigated. For many examples, the correct orientation was determined by smaller energy differences between parallel and antiparallel structures distributed over many residues and energy components. Prediction methods that used structure but incorporated varying approximations and assumptions showed quite different behaviors when used to investigate energetic contributions to orientation preference. Sequence based methods were sensitive to the choice of residue-pair interactions scored.     

Orientation and oligomerization specificity of the Bcr coiled-coil oligomerization domain

The Bcr oligomerization domain, from the Bcr-Abl oncoprotein, is an attractive therapeutic target for treating leukemias because it is required for cellular transformation. The domain homodimerizes via an antiparallel coiled coil with an adjacent short, helical swap domain. Inspection of the coiled-coil sequence does not reveal obvious determinants of helix-orientation specificity, raising the possibility that the antiparallel orientation preference and/or the dimeric oligomerization state are due to interactions of the swap domains. To better understand how structural specificity is encoded in Bcr, coiled-coil constructs containing either an N- or C-terminal cysteine were synthesized without the swap domain. When cross-linked to adopt exclusively parallel or antiparallel orientations, these showed similar circular dichroism spectra. Both constructs formed coiled-coil dimers, but the antiparallel construct was approximately 16 degrees C more stable than the parallel to thermal denaturation. Equilibrium disulfide-exchange studies confirmed that the isolated coiled-coil homodimer shows a very strong preference for the antiparallel orientation. We conclude that the orientation and oligomerization preferences of Bcr are not caused by the presence of the swap domains, but rather are directly encoded in the coiled-coil sequence. We further explored possible determinants of structural specificity by mutating residues in the d position of the coiled-coil core. Some of the mutations caused a change in orientation specificity, and all of the mutations led to the formation of higher-order oligomers. In the absence of the swap domain, these residues play an important role in disfavoring alternate states and are especially important for encoding dimeric oligomerization specificity.     

Septin ring size scaling and dynamics require the coiled-coil region of Shs1p

Septins are conserved GTP-binding proteins that assemble into heteromeric complexes that form filaments and higher-order structures in cells. What directs filament assembly, determines the size of higher-order septin structures, and governs septin dynamics is still not well understood. We previously identified two kinases essential for septin ring assembly in the filamentous fungus Ashbya gossypii and demonstrate here that the septin Shs1p is multiphosphorylated at the C-terminus of the protein near the predicted coiled-coil domain. Expression of the nonphosphorylatable allele shs1-9A does not mimic the loss of the kinase nor does complete truncation of the Shs1p C-terminus. Surprisingly, however, loss of the C-terminus or the predicted coiled-coil domain of Shs1p generates expanded zones of septin assemblies and ectopic septin fibers, as well as aberrant cell morphology. The expanded structures form coincident with ring assembly and are heteromeric. Interestingly, while septin recruitment to convex membranes is increased, septin localization is diminished at concave membranes in these mutants. Additionally, the loss of the coiled-coil leads to increased mobility of Shs1p. These data indicate the coiled-coil of Shs1p is an important negative regulator of septin ring size and mobility, and its absence may make septin assembly sensitive to local membrane curvature.     

Conformational specificity of the lac repressor coiled-coil tetramerization domain

Predictive understanding of how the folded, functional shape of a native protein is encoded in the linear sequence of its amino acid residues remains an unsolved challenge in modern structural biology. Antiparallel four-stranded coiled coils are relatively simple protein structures that embody a heptad sequence repeat and rich diversity for tertiary packing of alpha-helices. To explore specific sequence determinants of the lac repressor coiled-coil tetramerization domain, we have engineered a set of buried nonpolar side chains at the a-, d-, and e-positions into the hydrophobic interior of the dimeric GCN4 leucine zipper. Circular dichroism and equilibrium ultracentrifugation studies show that this core variant (GCN4-pAeLV) forms a stable tetrameric structure with a reversible and highly cooperative thermal unfolding transition. The X-ray crystal structure at 1.9 A reveals that GCN4-pAeLV is an antiparallel four-stranded coiled coil of the lac repressor type in which the a, d, and e side chains associate by means of combined knobs-against-knobs and knobs-into-holes packing with a characteristic interhelical offset of 0.25 heptad. Comparison of the side chain shape and packing in the antiparallel tetramers shows that the burial of alanine residues at the e positions between the neighboring helices of GCN4-pAeLV dictates both the antiparallel orientation and helix offset. This study fills in a gap in our knowledge of the determinants of structural specificity in antiparallel coiled coils and improves our understanding of how specific side chain packing forms the teritiary structure of a functional protein.     

Core residue replacements cause coiled-coil orientation switching in vitro and in vivo: structure-function correlations for osmosensory transporter ProP

Protein ProP acts as an osmosensory transporter in diverse bacteria. C-Terminal residues 468-497 of Escherichia coli ProP (ProPEc) form a four-heptad homodimeric alpha-helical coiled coil. Arg 488, at a core heptad a position, causes it to assume an antiparallel orientation. Arg in the hydrophobic core of coiled coils is destabilizing, but Arg 488 forms stabilizing interstrand salt bridges with Asp 475 and Asp 478. Mutation R488I destabilizes the coiled coil and elevates the osmotic pressure at which ProPEc activates. It may switch the coiled-coil orientation to parallel by eliminating the salt bridges and increasing the hydrophobicity of the core. In this study, mutations D475A and D478A, which disrupt the salt bridges without increasing the hydrophobicity of the coiled-coil core, had the expected modest impacts on the osmotic activation of ProPEc. The five-heptad coiled coil of Agrobacterium tumefaciens ProP (ProPAt) has K498 and R505 at a positions. Mutation K498I had little effect on the osmotic activation of ProPAt, and ProPAt-R505I was activated only at high osmotic pressure; on the other hand, the double mutant was refractory to osmotic activation. Both a synthetic peptide corresponding to ProPAt residues 478-516 and its K498I variant maintained the antiparallel orientation. The single R505I substitution created an unstable coiled coil with little orientation preference. Double mutation K498I/R505I switched the alignment, creating a stable parallel coiled coil. In vivo cross-linking showed that the C-termini of ProPAt and ProPAt-K498I/R505I were antiparallel and parallel, respectively. Thus, the antiparallel orientation of the ProP coiled coil is contingent on Arg in the hydrophobic core and interchain salt bridges. Two key amino acid replacements can convert it to a stable parallel structure, in vitro and in vivo. An intermolecular antiparallel coiled coil, present on only some orthologues, lowers the osmotic pressure required to activate ProP. Formation of a parallel coiled coil renders ProP inactive.     

X-ray structure of a water-soluble analog of the membrane protein phospholamban: sequence determinants defining the topology of tetrameric and pentameric coiled coils

Phospholamban (PLB) is a pentameric transmembrane protein that regulates the Ca(2+)-dependent ATPase SERCA2a in sarcoplasmic reticulum membranes. We previously described the computational design of a water-soluble variant of phospholamban, WSPLB, which reproduced many of the structural and functional properties of the native membrane-soluble protein. While the full-length WSPLB forms a pentamer in solution, a truncated variant forms very stable tetramers. To obtain insight into the tetramer-pentamer cytoplasmic switch, we solved the crystal structure of the truncated construct, WSPLB 21-52. This peptide has a heptad sequence repeat with Leu residues at a- and Ile at d-positions from residues 31-52. The crystal structure revealed that WSPLB 21-52 adopted an antiparallel tetrameric coiled coil. This topology contrasts with the parallel topology of an analogue of the coiled-coil of GCN4 with the same Leu(a) Ile(d) repeat. Analysis of these structures revealed how the nature of the partially exposed residues at e- and g-positions influence the topology formed by the bundle. We also constructed a model for the pentameric form of PLB using the coiled-coil parameters derived from a single monomer in the tetrameric structure. This model suggests that both buried and interfacial hydrogen bonds are important for stabilizing the parallel pentamer.     

Antiparallel orientation of the two double-stranded coiled-coils in the tetrameric protofilament unit of intermediate filaments

The chymotryptically excised middle domain of desmin slightly exceeds in length the structurally conserved alpha-helical middle region documented in all intermediate filament proteins by amino acid sequence data. This rod domain is a protofilament derivative with a tetrameric organization, thus indicating the presence of two double-stranded coiled-coil units. We now show by immunoelectron microscopy that Fab fragments of a desmin-specific monoclonal antibody mixed with the rod lead to dumb-bell-shaped structures. The tagging of both ends together with the length of the rod (48 nm) argues for an antiparallel orientation of the two coiled-coils without a major stagger. This information combined with the lateral 21 nm periodicity of the intermediate filament observed by us and others leads to a structural hypothesis similar to those entertained from X-ray data on wool alpha-keratins, although here an antiparallel tetrameric unit of some 60 to 66 nm is invoked, which has never been isolated. The structure that we discuss allows for the existence of both the particles, and the antibody experiment strongly supports the antiparallel orientation postulated in both approaches. The tube-like filament structure proposed for the intermediate filament agrees with recent mass per unit length measurements and allows for two minor classes of intermediate filaments with different values in this property as also found experimentally.     

Structural analysis of smooth muscle tropomyosin α and β isoforms

A large number of tropomyosin (Tm) isoforms function as gatekeepers of the actin filament, controlling the spatiotemporal access of actin-binding proteins to specialized actin networks. Residues ∼40–80 vary significantly among Tm isoforms, but the impact of sequence variation on Tm structure and interactions with actin is poorly understood, because structural studies have focused on skeletal muscle Tmα. We describe structures of N-terminal fragments of smooth muscle Tmα and Tmβ (sm-Tmα and sm-Tmβ). The 2.0-Å structure of sm-Tmα81 (81-aa) resembles that of skeletal Tmα, displaying a similar super-helical twist matching the contours of the actin filament. The 1.8-Å structure of sm-Tmα98 (98-aa) unexpectedly reveals an antiparallel coiled coil, with the two chains staggered by only 4 amino acids and displaying hydrophobic core interactions similar to those of the parallel dimer. In contrast, the 2.5-Å structure of sm-Tmβ98, containing Gly-Ala-Ser at the N terminus to mimic acetylation, reveals a parallel coiled coil. None of the structures contains coiled-coil stabilizing elements, favoring the formation of head-to-tail overlap complexes in four of five crystallographically independent parallel dimers. These complexes show similarly arranged 4-helix bundles stabilized by hydrophobic interactions, but the extent of the overlap varies between sm-Tmβ98 and sm-Tmα81 from 2 to 3 helical turns. The formation of overlap complexes thus appears to be an intrinsic property of the Tm coiled coil, with the specific nature of hydrophobic contacts determining the extent of the overlap. Overall, the results suggest that sequence variation among Tm isoforms has a limited effect on actin binding but could determine its gatekeeper function.     

Multicoil2: predicting coiled coils and their oligomerization states from sequence in the twilight zone

The alpha-helical coiled coil can adopt a variety of topologies, among the most common of which are parallel and antiparallel dimers and trimers. We present Multicoil2, an algorithm that predicts both the location and oligomerization state (two versus three helices) of coiled coils in protein sequences. Multicoil2 combines the pairwise correlations of the previous Multicoil method with the flexibility of Hidden Markov Models (HMMs) in a Markov Random Field (MRF). The resulting algorithm integrates sequence features, including pairwise interactions, through multinomial logistic regression to devise an optimized scoring function for distinguishing dimer, trimer and non-coiled-coil oligomerization states; this scoring function is used to produce Markov Random Field potentials that incorporate pairwise correlations localized in sequence. Multicoil2 significantly improves both coiled-coil detection and dimer versus trimer state prediction over the original Multicoil algorithm retrained on a newly-constructed database of coiled-coil sequences. The new database, comprised of 2,105 sequences containing 124,088 residues, includes reliable structural annotations based on experimental data in the literature. Notably, the enhanced performance of Multicoil2 is evident when tested in stringent leave-family-out cross-validation on the new database, reflecting expected performance on challenging new prediction targets that have minimal sequence similarity to known coiled-coil families. The Multicoil2 program and training database are available for download from http://multicoil2.csail.mit.edu.     

Intermediate filament structure: 1. Analysis of IF protein sequence data

Amino acid sequence data for intermediate filament proteins have been analysed with a view to identifying structurally invariant segments and determining their likely secondary structure. The sequences in these segments have also been analysed for periodic distributions of particular types of residue. The results support the classification of intermediate filament proteins into three main groups and also reinforce the concept of a molecular structure with a central domain of coiled-coil segments, together with essentially non-helical N-terminal and C-terminal domains of variable size and composition. Regions exhibiting the greatest homology between the three types of IF chain are identified and significant variation in charged residue disposition along the length of individual chains is noted. The conservation in all IF protein chains of specific sites of coiled-coil rope interruption are discussed in terms of the probable molecular structure. Stabilizing ionic interactions between coiled-coil chain segments have been investigated quantitatively as a function of the relative chain stagger. In all cases and calculations favour ropes in which the constituent chains are in-register and parallel rather than antiparallel.     

Detection of alpha-helical coiled-coil dimer formation by spin-labeled synthetic peptides: a model parallel coiled-coil peptide and the antiparallel coiled coil formed by a replica of the ProP C-terminus

Electron paramagnetic resonance spectroscopy was used to determine relative peptide orientation within homodimeric, alpha-helical coiled-coil structures. Introduction of cysteine (Cys) residues into peptides/proteins for spin labeling allows detection of their oligomerization from exchange broadening or dipolar interactions between residues within 25 A of each other. Two synthetic peptides containing Cys substitutions were used: a 35-residue model peptide and the 30-residue ProP peptide. The model peptide is known to form a stable, parallel homodimeric coiled coil, which is partially destabilized by Cys substitutions at heptad a and d positions (peptides C30a and C33d). The ProP peptide, a 30-residue synthetic peptide, corresponds to residues 468-497 of osmoregulatory transporter ProP from Escherichia coli. It forms a relatively unstable, homodimeric coiled coil that is predicted to be antiparallel in orientation. Cys was introduced in heptad g positions of the ProP peptide, near the N-terminus (K473C, creating peptide C473g) or closer to the center of the sequence (E480C, creating peptide C480g). In contrast to the destabilizing effect of Cys substitution at the core heptad a or d positions of model peptides C30a and C33d, circular dichroism spectroscopy showed that Cys substitutions at the heptad g positions of the ProP peptide had little or no effect on coiled-coil stability. Thermal denaturation analysis showed that spin labeling increased the stability of the coiled coil for all peptides. Strong exchange broadening was detected for both C30a and C33d, in agreement with a parallel structure. EPR spectra of C480g had a large hyperfine splitting of about 90 G, indicative of strong dipole-dipole interactions and a distance between spin-labeled residues of less than 9 A. Spin-spin interactions were much weaker for C473g. These results supported the hypothesis that the ProP peptide primarily formed an antiparallel coiled coil, since formation of a parallel dimer should result in similar spin-spin interactions for the spin-labeled Cys at both sites.     

Protein-protein interactions governing septin heteropentamer assembly and septin filament organization in Saccharomyces cerevisiae

Mitotic yeast (Saccharomyces cerevisiae) cells express five related septins (Cdc3, Cdc10, Cdc11, Cdc12, and Shs1) that form a cortical filamentous collar at the mother-bud neck necessary for normal morphogenesis and cytokinesis. All five possess an N-terminal GTPase domain and, except for Cdc10, a C-terminal extension (CTE) containing a predicted coiled coil. Here, we show that the CTEs of Cdc3 and Cdc12 are essential for their association and for the function of both septins in vivo. Cdc10 interacts with a Cdc3-Cdc12 complex independently of the CTE of either protein. In contrast to Cdc3 and Cdc12, the Cdc11 CTE, which recruits the nonessential septin Shs1, is dispensable for its function in vivo. In addition, Cdc11 forms a stoichiometric complex with Cdc12, independent of its CTE. Reconstitution of various multiseptin complexes and electron microscopic analysis reveal that Cdc3, Cdc11, and Cdc12 are all necessary and sufficient for septin filament formation, and presence of Cdc10 causes filament pairing. These data provide novel insights about the connectivity among the five individual septins in functional septin heteropentamers and the organization of septin filaments.     

Symmetry of septin hourglass and ring structures

Septin filaments form ordered hourglass and ring-shaped structures in close apposition to the yeast bud-neck membrane. The septin hourglass scaffolds the asymmetric localization of many essential cell division proteins. However, it is unknown whether the septin structures have an overall polarity along the mother-daughter axis that determines the asymmetric protein localization. Here we engineered rigid septin- green fluorescent protein (GFP) fusions with various fluorescence dipole directions by changing the position of the GFP beta-barrel relative to the septin filament axis. We then used polarized fluorescence microscopy to detect potential asymmetries in the filament organization. We found that both the hourglass and ring filament assemblies have sub-resolution C(2) symmetry and lack net polarity along the mother-daughter axis. The hourglass filaments have an additional degree of symmetry relative to the ring filaments, most likely due to a twist in their higher-order structure. We previously reported that during the hourglass to rings transition septin filaments change their direction. Here we show that the filaments also undergo a change in their lateral organization, consistent with filament untwisting. The lack of net septin polarity along the mother-daughter axis suggests that there are no septin-based structural reasons for the observed asymmetry of other proteins. We discuss possible anisotropic processes that could break the septin symmetry and establish the essential bud-neck asymmetry.     

Structures and polymorphic interactions of two heptad-repeat regions of the SARS virus S2 protein

Entry of SARS coronavirus into its target cell requires large-scale structural transitions in the viral spike (S) glycoprotein in order to induce fusion of the virus and cell membranes. Here we describe the identification and crystal structures of four distinct alpha-helical domains derived from the highly conserved heptad-repeat (HR) regions of the S2 fusion subunit. The four domains are an antiparallel four-stranded coiled coil, a parallel trimeric coiled coil, a four-helix bundle, and a six-helix bundle that is likely the final fusogenic form of the protein. When considered together, the structural and thermodynamic features of the four domains suggest a possible mechanism whereby the HR regions, initially sequestered in the native S glycoprotein spike, are released and refold sequentially to promote membrane fusion. Our results provide a structural framework for understanding the control of membrane fusion and should guide efforts to intervene in the SARS coronavirus entry process.