Formation of an antiparallel, intermolecular coiled coil is associated with in vivo dimerization of osmosensor and osmoprotectant transporter ProP in Escherichia coli

Membrane transporter ProP from Escherichia coli senses extracellular osmolality and responds by mediating the uptake of osmoprotectants such as glycine betaine when osmolality is high. Earlier EPR and NMR studies showed that a peptide replica of the cytoplasmic ProP carboxyl terminus (residues D468-R497) forms a homodimeric, antiparallel, alpha-helical coiled coil in vitro stabilized by electrostatic interactions involving R488. Amino acid replacement R488I disrupted coiled-coil formation by the ProP peptide, elevated the osmolality at which ProP became active, and rendered the osmolality response of ProP transient. In the present study, either E480 or K473 was replaced with cysteine (Cys) in ProP, a Cys-less, fully functional, histidine-tagged ProP variant, to use Cys-specific cross-linking approaches to determine if antiparallel coiled-coil formation and dimerization of the intact protein occur in vivo. The Cys at positions 480 would be closer in an antiparallel dimer than those at positions 473. These replacements did not disrupt coiled-coil formation by the ProP peptide. Partial homodimerization of variant ProP-E480C could be demonstrated in vivo and in membrane preparations via Cys-specific cross-linking with dithiobis(maleimidoethane) or by Cys oxidation to cystine by copper phenanthroline. In contrast, these reagents did not cross-link ProP with Cys at position 133 or 241. Cross-linking of ProP with Cys at position 473 was limited and occurred only if ProP was overexpressed, consistent with an antiparallel orientation of the coiled coil in the intact protein in vivo. Although replacement E480C did not alter transporter activity, replacement K473C reduced the extent and elevated the threshold for osmotic activation. K473 may play a role in ProP structure and function that is not reflected in altered coiled-coil formation by the corresponding peptide. Substitution R488I affected the activities of ProP-(His)(6), ProP-E480C, and ProP-K473C as it affected the activity of ProP. Surprisingly, it did not eliminate cross-linking of Cys at position 480, and it elevated cross-linking at position 473, even when ProP was expressed at physiological levels. This suggested that the R488I substitution may have changed the relative orientation of the C-termini within the dimeric protein from antiparallel to parallel, resulting in only transient osmotic activation. These results suggest that ProP is in monomer-dimer equilibrium in vivo. Dimerization may be mediated by C-terminal coiled-coil formation and/or by interactions between other structural domains, which in turn facilitate C-terminal coiled-coil formation. Antiparallel coiled-coil formation is required for activation of ProP at low osmolality.     

The osmotic activation of transporter ProP is tuned by both its C-terminal coiled-coil and osmotically induced changes in phospholipid composition

Transporter ProP of Escherichia coli (ProPEc) senses extracellular osmolality and mediates osmoprotectant uptake when it is rising or high. A replica of the ProPEc C terminus (Asp468-Arg497) forms an intermolecular alpha-helical coiled-coil. This structure is implicated in the osmoregulation of intact ProPEc, in vivo. Like that from Corynebacterium glutamicum (ProPCg), the ProP orthologue from Agrobacterium tumefaciens (ProPAt) sensed and responded to extracellular osmolality after expression in E. coli. The osmotic activation profiles of all three orthologues depended on the osmolality of the bacterial growth medium, the osmolality required for activation rising as the growth osmolality approached 0.7 mol/kg. Thus, each could undergo osmotic adaptation. The proportion of cardiolipin in a polar lipid extract from E. coli increased with extracellular osmolality so that the osmolality activating ProPEc was a direct function of membrane cardiolipin content. Group A ProP orthologues (ProPEc, ProPAt) share the C-terminal coiled-coil domain and were activated at low osmolalities. Like variant ProPEc-R488I, in which the C-terminal coiled-coil is disrupted, ProPEc derivatives that lack the coiled-coil and Group B orthologue ProPCg required a higher osmolality to activate. The amplitude of ProPEc activation was reduced 10-fold in its deletion derivatives. The coiled-coil structure is not essential for osmotic activation of ProP per se. However, it tunes Group A orthologues to osmoregulate over a low osmolality range. Coiled-coil lesions may impair both coiled-coil formation and interaction of ProPEc with amplifier protein ProQ. Cardiolipin may contribute to ProP adaptation by altering bulk membrane properties or by acting as a ProP ligand.     

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.     

Solution structure of the C-terminal antiparallel coiled-coil domain from Escherichia coli osmosensor ProP

Bacteria respond to increasing medium osmolality by accumulating organic solutes that are compatible with cellular functions. Transporter ProP of Escherichia coli, a proton symporter and a member of the major facilitator superfamily, senses osmotic shifts and responds by importing osmolytes such as glycine betaine. ProP contains a cytoplasmic, C-terminal extension that is essential for its activity. A peptide corresponding to the C-terminal extension of ProP forms a homodimeric alpha-helical coiled-coil even though some of its heptad a positions are not occupied by hydrophobic amino acid residues. Unexpectedly, amino acid replacement R488I, occurring at a heptad a position, destabilized the coiled-coil formed by the ProP peptide and attenuated the response of the intact transporter to osmotic upshifts in vivo. Thus, ProP was proposed to dimerize via an antiparallel coiled-coil. We used nuclear magnetic resonance (NMR) spectroscopy to determine the structure of the synthetic peptide corresponding to residues 468-497 of ProP. This region did form an antiparallel coil-coil in which critical residue R488 specifies the antiparallel coiled-coil orientation by forming stabilizing salt-bridges. Charged residues (both acidic and basic) are clustered on the c/g surface of the coiled-coil whereas polar residues are distributed on the b/e surface. This causes the structure to be bent, in contrast to other known antiparallel coiled-coils (those from the hepatitis delta antigen (PDB ID code 1A92) and the bovine F(1) ATPase inhibitor protein (PDB ID code 1HF9)). The coiled-coil and its possible importance for osmosensing are discussed.     

The role of the carboxyl terminal alpha-helical coiled-coil domain in osmosensing by transporter ProP of Escherichia coli

Concentrative uptake of osmoprotectants via transporter ProP contributes to the rehydration of Escherichia coli cells that encounter high osmolality media. A member of the major facilitator superfamily, ProP is activated by osmotic upshifts in whole bacteria, in cytoplasmic membrane vesicles and in proteoliposomes prepared with the purified protein. Soluble protein ProQ is also required for full osmotic activation of ProP in vivo. ProP is differentiated from structural and functional homologues by its osmotic activation and its C-terminal extension, which is predicted to form an alpha-helical coiled-coil. A synthetic polypeptide corresponding to the C-terminus of ProP (ProP-p) formed a dimeric alpha-helical coiled-coil. A derivative of transporter ProP lacking 26 C-terminal amino acids was expressed but inactive. A derivative harbouring amino acid changes K460I, Y467I and H495I (each at the core, coiled-coil 'a' position) required a larger osmotic upshift for activation than did the wild type transporter. The same changes extended, stabilized and altered the oligomeric state of the coiled-coil formed by ProP-p. Amino acid change R488I (also at the 'a' position) further increased the magnitude of the osmotic upshift required to activate ProP, reduced the activity attained and rendered ProP activation transient. Unexpectedly, replacement R488I destabilized the coiled-coil formed by ProP-p. The activity and osmotic activation of ProP were even more strongly attenuated by helix-destabilizing change I474P. These data demonstrate that the carboxyl terminal domain of ProP can form a homodimeric alpha-helical coiled-coil with unusual properties. They implicate the C-terminal domain in the osmotic activation of ProP.     

Orientational Ambiguity in Septin Coiled Coils and its Structural Basis

Septins are an example of subtle molecular recognition whereby different paralogues must correctly assemble into functional filaments important for essential cellular events such as cytokinesis. Most possess C-terminal domains capable of forming coiled coils which are believed to be involved in filament formation and bundling. Here, we report an integrated structural approach which aims to unravel their architectural diversity and in so doing provide direct structural information for the coiled-coil regions of five human septins. Unexpectedly, we encounter dimeric structures presenting both parallel and antiparallel arrangements which are in consonance with molecular modelling suggesting that both are energetically accessible. These sequences therefore code for two metastable states of different orientations which employ different but overlapping interfaces. The antiparallel structures present a mixed coiled-coil interface, one side of which is dominated by a continuous chain of core hydrophilic residues. This unusual type of coiled coil could be used to expand the toolkit currently available to the protein engineer for the design of previously unforeseen coiled-coil based assemblies. Within a physiological context, our data provide the first atomic details related to the assumption that the parallel orientation is likely formed between septin monomers from the same filament whilst antiparallelism may participate in the widely described interfilament cross bridges necessary for higher order structures and thereby septin function.     

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.     

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.     

Removing an interhelical salt bridge abolishes coiled-coil formation in a de novo designed peptide

Alpha-helical coiled coils represent a common protein oligomerization motif that are mainly stabilized by hydrophobic interactions occurring along their coiled-coil interface, the so-called hydrophobic seam. We have recently de novo designed and optimized a series of two-heptad repeat long coiled-coil peptides which are further stabilized by a complex network of inter- and intrahelical salt bridges. Here we have extended the de novo design of such two heptad-repeat long peptides by removing the central and most important g-e' Arg to Glu (g-e'RE) ionic interhelical interaction and replacing these residues by alanine residues. The effect of the missing interhelical ionic interaction on coiled-coil formation and stability has been analyzed by CD spectroscopy, analytical ultracentrifugation, and X-ray crystallography. We show that the peptide, while being highly alpha-helical, is no longer able to form a parallel coiled-coil structure but rather assumes an octameric globular helical assembly devoid of any coiled-coil interactions.     

Computational analysis of residue contributions to coiled-coil topology

A variety of features are thought to contribute to the oligomeric and topological specificity of coiled coils. In previous work, we examined the determinants of oligomeric state. Here, we examine the energetic basis for the tendency of six coiled-coil peptides to align their α-helices in antiparallel orientation using molecular dynamics simulations with implicit solvation (EEF1.1). We also examine the effect of mutations known to disrupt the topology of these peptides. In agreement with experiment, ARG or LYS at a or d positions were found to stabilize the antiparallel configuration. The modeling suggests that this is not due to a-a' or d-d' repulsions but due to interactions with e' and g' residues. TRP at core positions also favors the antiparallel configuration. Residues that disfavor parallel dimers, such as ILE at d, are better tolerated in, and thus favor the antiparallel configuration. Salt bridge networks were found to be more stabilizing in the antiparallel configuration for geometric reasons: antiparallel helices point amino acid side chains in opposite directions. However, the structure with the largest number of salt bridges was not always the most stable, due to desolvation and configurational entropy contributions. In tetramers, the extent of stabilization of the antiparallel topology by core residues is influenced by the e' residue on a neighboring helix. Residues at b and c positions in some cases also contribute to stabilization of antiparallel tetramers. This work provides useful rules toward the goal of designing coiled coils with a well-defined and predictable three-dimensional structure.     

Crystal structure of a naturally occurring parallel right-handed coiled coil tetramer

The crystal structure of a polypeptide chain fragment from the surface layer protein tetrabrachion from Staphylothermus marinus has been determined at 1.8 A resolution. As proposed on the basis of the presence of 11-residue repeats, the polypeptide chain fragment forms a parallel right-handed coiled coil structure. Complementary hydrophobic interactions and complex networks of surface salt bridges result in an extremely thermostable tetrameric structure with remarkable properties. In marked contrast to left-handed coiled coil tetramers, the right-handed coiled coil reveals large hydrophobic cavities that are filled with water molecules. As a consequence, the packing of the hydrophobic core differs markedly from that of a right-handed parallel coiled coil tetramer that was designed on the basis of left-handed coiled coil structures.     

How does a registry change in dynein's coiled-coil stalk drive binding of dynein to microtubules?

Dynein is a motor protein that transports cellular cargo along the microtubule (MT) by consuming ATP. Dynein's microtubule-binding domain (MTBD) is separated from the ATP-binding core by a ~15 nm stalk that consists of two α-helices forming an antiparallel coiled coil. It was previously suggested that the coiled-coil stalk creates a registry shift to modulate its binding affinity for MT. A crystal structure of the low-affinity form of MTBD was determined, but that of the high-affinity form with the registry shift is not yet available. In this study, we obtained an all-atom model structure for the high-affinity form of MTBD bound to MT by an anisotropic network model, protein-protein docking, and molecular dynamics simulations. We observe that the magnitude of the coiled-coil helix sliding is dramatically reduced near the two prolines that form the stalk-MTBD boundary and subsequently transformed to cyclic movements of MTBD helices, leading to formation of a new salt bridge with MT at the binding interface. The proposed mechanism explains the roles of highly conserved residues such as the two prolines at the stalk-MTBD boundary, the nonpolar tryptophan and proline residues near the binding interface, and the electropositive residues forming salt bridges with MT.     

Kinking the coiled coil--negatively charged residues at the coiled-coil interface

The coiled coil is one of the most common protein-structure motifs. It is believed to be adopted by 3-5% of all amino acids in proteins. It comprises two or more alpha-helical chains wrapped around one another. The sequences of most coiled coils are characterized by a seven-residue (heptad) repeat, denoted (abcdefg)(n). Residues at the a and d positions define the helical interface (core) and are usually hydrophobic, though about 20% are polar or charged. We show that parallel coiled-coils have a unique pattern of their negatively charged residues at the core positions: aspartic acid is excluded from these positions while glutamic acid is not. In contrast the antiparallel structures are more permissive in their amino acid usage. We show further, and for the first time, that incorporation of Asp but not Glu into the a positions of a parallel coiled coil creates a flexible hinge and that the maximal hinge angle is being directly related to the number of incorporated mutations. These new computational and experimental observations will be of use in improving protein-structure predictions, and as rules to guide rational design of novel coiled-coil motifs and coiled coil-based materials.     

A distinct 14 residue site triggers coiled-coil formation in cortexillin I.

We have investigated the process of the assembly of the Dictyostelium discoideum cortexillin I oligomerization domain (Ir) into a tightly packed, two-stranded, parallel coiled-coil structure using a variety of recombinant polypeptide chain fragments. The structures of these Ir fragments were analyzed by circular dichroism spectroscopy, analytical ultracentrifugation and electron microscopy. Deletion mapping identified a distinct 14 residue site within the Ir coiled coil, Arg311-Asp324, which was absolutely necessary for dimer formation, indicating that heptad repeats alone are not sufficient for stable coiled-coil formation. Moreover, deletion of the six N-terminal heptad repeats of Ir led to the formation of a four- rather than a two-helix structure, suggesting that the full-length cortexillin I coiled-coil domain behaves as a cooperative folding unit. Most interestingly, a 16 residue peptide containing the distinct coiled-coil 'trigger' site Arg311-Asp324 yielded approximately 30% helix formation as monomer, in aqueous solution. pH titration and NaCl screening experiments revealed that the peptide's helicity depends strongly on pH and ionic strength, indicating that electrostatic interactions by charged side chains within the peptide are critical in stabilizing its monomer helix. Taken together, these findings demonstrate that Arg311-Asp324 behaves as an autonomous helical folding unit and that this distinct Ir segment controls the process of coiled-coil formation of cortexillin I.     

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.     

Cardiolipin controls the osmotic stress response and the subcellular location of transporter ProP in Escherichia coli

The phospholipid composition of the membrane and transporter structure control the subcellular location and function of osmosensory transporter ProP in Escherichia coli. Growth in media of increasing osmolality increases, and entry to stationary phase decreases, the proportion of phosphatidate in anionic lipids (phosphatidylglycerol (PG) plus cardiolipin (CL)). Both treatments increase the CL:PG ratio. Transporters ProP and LacY are concentrated with CL (and not PG) near cell poles and septa. The polar concentration of ProP is CL-dependent. Here we show that the polar concentration of LacY is CL-independent. The osmotic activation threshold of ProP was directly proportional to the CL content of wild type bacteria, the PG content of CL-deficient bacteria, and the anionic lipid content of cells and proteoliposomes. CL was effective at a lower concentration in cells than in proteoliposomes, and at a much lower concentration than PG in either system. Thus, in wild type bacteria, osmotic induction of CL synthesis and concentration of ProP with CL at the cell poles adjust the osmotic activation threshold of ProP to match ambient conditions. ProP proteins linked by homodimeric, C-terminal coiled-coils are known to activate at lower osmolalities than those without such structures and coiled-coil disrupting mutations raise the osmotic activation threshold. Here we show that these mutations also prevent polar concentration of ProP. Stabilization of the C-terminal coiled-coil by covalent cross-linking of introduced Cys reverses the impact of increasing CL on the osmotic activation of ProP. Association of ProP C termini with the CL-rich membrane at cell poles may raise the osmotic activation threshold by blocking coiled-coil formation. Mutations that block coiled-coil formation may also block association of the C termini with the CL-rich membrane.     

The use of coiled-coil interactions for the analysis and micropreparative isolation of adenomatous polyposis coli protein complexes.

The coiled coil is a common structural motif found both as the dominant structure in fibrous proteins and as an oligomerization domain in a variety of cytoskeletal and extracellular matrix proteins. Coiled-coils typically consist of two to four helices that are supercoiled around one another in either parallel or antiparallel orientations. In the past few years our knowledge of the structure and specificity of coiled coil interactions has increased, allowing the de novo design and preparation of coiled-coils with well-defined structure and specificity. Indeed, the design and synthesis of a peptide that binds specifically to a single coiled-coil-containing protein, adenomatous polyposis coli (APC) has been reported. We have optimized solid-phase synthesis techniques to produce a modified form of the anti-APC peptide that contains a biotin moiety specifically placed so as to allow selective orientation onto the surface of a biosensor or affinity support. These peptide surfaces have been used to both monitor and purify APC and APC complexes from cellular extracts.     

The coiled-coil trigger site of the rod domain of cortexillin I unveils a distinct network of interhelical and intrahelical salt bridges

BACKGROUND: The parallel two-stranded alpha-helical coiled coil is the most frequently encountered subunit-oligomerization motif in proteins. The simplicity and regularity of this motif have made it an attractive system to explore some of the fundamental principles of protein folding and stability and to test the principles of de novo design. RESULTS: The X-ray crystal structure of the 18-heptad-repeat alpha-helical coiled-coil domain of the actin-bundling protein cortexillin I from Dictyostelium discoideum is a tightly packed parallel two-stranded alpha-helical coiled coil. It harbors a distinct 14-residue sequence motif that is essential for coiled-coil formation, and is a prerequisite for the assembly of cortexillin I. The atomic structure reveals novel types of ionic coiled-coil interactions. In particular, the structure shows that a characteristic interhelical and intrahelical salt-bridge pattern, in combination with the hydrophobic interactions occurring at the dimer interface, is the key structural feature of its coiled-coil trigger site. CONCLUSIONS: The knowledge gained from the structure could be used in the de novo design of alpha-helical coiled coils for applications such as two-stage drug targeting and delivery systems, and in the design of coiled coils as templates for combinatorial helical libraries in drug discovery and as synthetic carrier molecules.     

The affinity of the dynein microtubule-binding domain is modulated by the conformation of its coiled-coil stalk

The microtubule-binding domain (MTBD) of dynein is separated from the AAA (ATPase with any other activity) core of the motor by an approximately 15-nm stalk that is predicted to consist of an antiparallel coiled coil. However, the structure of this coiled coil and the mechanism it uses to mediate communication between the MTBD and ATP-binding core are unknown. Here, we sought to identify the optimal alignment between the hydrophobic heptad repeats in the two strands of the stalk coiled coil. To do this, we fused the MTBD of mouse cytoplasmic dynein, together with 12-36 residues of its stalk, onto a stable coiled-coil base provided by Thermus thermophilus seryl-tRNA synthetase and tested these chimeric constructs for microtubule binding in vitro. The results identified one alignment that yielded a protein displaying high affinity for microtubules (2.2 microM). The effects of mutations applied to the MTBD of this construct paralleled those previously reported (Koonce, M. P., and Tikhonenko, I. (2000) Mol. Biol. Cell 11, 523-529) for an intact dynein motor unit in the absence of ATP, suggesting that it resembles the tight binding state of native intact dynein. All other alignments showed at least 10-fold lower affinity for microtubules with the exception of one, which had an intermediate affinity. Based on these results and on amino acid sequence analysis, we hypothesize that dynein utilizes small amounts of sliding displacement between the two strands of its coiled-coil stalk as a means of communication between the AAA core of the motor and the MTBD during the mechanochemical cycle.     

A molecular dynamics study of the formation, stability, and oligomerization state of two designed coiled coils: possibilities and limitations

The formation, relative stability, and possible stoichiometries of two (self-)complementary peptide sequences (B and E) designed to form either a parallel homodimeric (B + B) or an antiparallel heterodimeric (B + E) coiled coil have been investigated. Peptide B shows a characteristic coiled coil pattern in circular dichroism spectra at pH 7.4, whereas peptide E is apparently random coiled under these conditions. The peptides are complementary to each other, with peptide E forming a coiled coil when mixed with peptide B. Molecular dynamics simulations show that combinations of B + B and B + E readily form a dimeric coiled coil, whereas E + E does not fall in line with the experimental data. However, the simulations strongly suggest the preferred orientation of the helices in the homodimeric coiled coil is antiparallel, with interactions at the interface quite different to that of the idealized model. In addition, molecular dynamics simulations suggest equilibrium between dimers, trimers, and tetramers of alpha-helices for peptide B.