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.     

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.     

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.     

Sliding Mechanism at a Coiled-Coil Interface

The α-helical coiled coil (CC) is a common protein motif that because of the simplicity of its sequence/structure relationship, it has been studied extensively to address fundamental questions in protein science as well as to develop strategies for designing protein with novel architectures. Nevertheless, a complete understanding of CC structures and their dynamics is still far from achieved. Particularly, spontaneous sliding at interfaces of CC proteins was observed for some systems, but its mechanism and usage as an intrinsic conformational change at CCs in protein-protein interfaces is unclear. Using coarse-grained and atomistic simulations, we study various sequences of homodimeric CC, in both parallel and antiparallel configurations. Both the strength of the hydrophobic core and the existence of salt bridges at the periphery of the interface affect sliding dynamics at the CC interface. Although the energy landscape for sliding along a CC interface is different for parallel and antiparallel configurations, both are characterized by a free energy of 1–1.5 kcal/mol, depending on the residues that constitute the CC interface. These barrier heights suggest that sliding kinetics is relatively slow in CC systems and are not expected to be of long length scale, yet they can be involved in functional motions. Our study explains the sliding that has been experimentally observed for the antiparallel CC of the dynein stalk region and the nuclear pore complex and suggests that this one-dimensional motion is an intrinsic feature in CC systems that can be involved in other CC systems.     

Structural basis for paramyxovirus-mediated membrane fusion

Paramyxoviruses are responsible for significant human mortality and disease worldwide, but the molecular mechanisms underlying their entry into host cells remain poorly understood. We have solved the crystal structure of a fragment of the simian parainfluenza virus 5 fusion protein (SV5 F), revealing a 96 A long coiled coil surrounded by three antiparallel helices. This structure places the fusion and transmembrane anchor of SV5 F in close proximity with a large intervening domain at the opposite end of the coiled coil. Six amino acids, potentially part of the fusion peptide, form a segment of the central coiled coil, suggesting that this structure extends into the membrane. Deletion mutants of SV5 F indicate that putative flexible tethers between the coiled coil and the viral membrane are dispensable for fusion. The lack of flexible tethers may couple a final conformational change in the F protein directly to the fusion of two bilayers.     

Structure and catalytic activation of the TRIM23 RING E3 ubiquitin ligase

Tripartite motif (TRIM) proteins comprise a large family of RING‐type ubiquitin E3 ligases that regulate important biological processes. An emerging general model is that TRIMs form elongated antiparallel coiled‐coil dimers that prevent interaction of the two attendant RING domains. The RING domains themselves bind E2 conjugating enzymes as dimers, implying that an active TRIM ligase requires higher‐order oligomerization of the basal coiled‐coil dimers. Here, we report crystal structures of the TRIM23 RING domain in isolation and in complex with an E2–ubiquitin conjugate. Our results indicate that TRIM23 enzymatic activity requires RING dimerization, consistent with the general model of TRIM activation.     

Computational assessment of folding energy landscapes in heterodimeric coiled coils

The coiled coil structural motif consists of alpha helices supercoiling around each other to form staggered knobs‐into‐holes packing. Such structures are deceptively simple, especially as they often can be described with parametric equations, but are known to exist in various conformations. Even the simplest systems, consisting of 2 monomers, can assemble into a wide range of states. They can form canonical as well as noncanonical coiled coils, be parallel or antiparallel, where helices associate with different degrees of shift, tilt, and rotation. Here, we investigate the energy landscape of heterodimeric coiled coils by carrying out de novo folding simulations starting from amino acid sequence. We folded a diverse set of 22 heterodimers and demonstrate that the approach is capable of identifying the atomic details in the experimental structure in the majority of cases. Our methodology also enables exploration of alternative states that can be accessible in solution beyond the experimentally determined structure. For many systems, we observe folding energy landscapes with multiple energy minima and several isoenergetic states. By comparing coiled coils from single domains and those extracted from larger proteins, we find that standalone coiled coils have deeper energy wells at the experimentally determined conformation. By folding the competing homodimeric states in addition to the heterodimers, we observe that the structural specificity towards the heteromeric state is often small. Taken together, our results demonstrate that de novo folding simulations can be a powerful tool to characterize structural specificity of coiled coils when coupled to assessment of energy landscapes.     

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.     

Dissecting the assembly of Abeta16-22 amyloid peptides into antiparallel beta sheets

Multiple long molecular dynamics simulations are used to probe the oligomerization mechanism of Abeta(16-22) (KLVFFAE) peptides. The peptides, in the monomeric form, adopt either compact random-coil or extended beta strand-like structures. The assembly of the low-energy oligomers, in which the peptides form antiparallel beta sheets, occurs by multiple pathways with the formation of an obligatory alpha-helical intermediate. This observation and the experimental results on fibrillogenesis of Abeta(1-40) and Abeta(1-42) peptides suggest that the assembly mechanism (random coil --> alpha helix --> beta strand) is universal for this class of peptides. In Abeta(16-22) oligomers both interpeptide hydrophobic and electrostatic interactions are critical in the formation of the antiparallel beta sheet structure. Mutations of either hydrophobic or charged residues destabilize the oligomer, which implies that the 16-22 fragments of Arctic (E22G), Dutch (E22Q), and Italian (E22K) mutants are unlikely to form ordered fibrils.     

Side-chains configurations in coiled coils revealed by the 5.15-A meridional reflection on hard alpha-keratin X-ray diffraction patterns

The origin of the 5.15-A meridional reflection on hard alpha-keratin X-ray diffraction patterns is discussed in terms of side-chains conformations. We show it to reveal specific configurations of the side chains which are common to all two-stranded alpha-helical coiled coils. Combining literature data on crystallised coiled coil pieces and molecular dynamics results with our X-ray diffraction pattern simulations, we propose rules for the attribution of chi1 torsion angles for coiled coils involved in fibres whose structure cannot be resolved at atomic resolution: in a (a b c d e f g) heptad repeat, a and d residues, respectively, adopt mean t and g+ configurations, whereas statistical rules are given for the other residues.     

Metallopolymer-peptide conjugates: synthesis and self-assembly of polyferrocenylsilane graft and block copolymers containing a beta-sheet forming Gly-Ala-Gly-Ala tetrapeptide segment

We describe the synthesis and self-assembly of two beta-sheet forming metallopolymer-peptide conjugates. The ability of the oligotetrapeptide sequence Gly-Ala-Gly-Ala (GAGA) to form antiparallel beta-sheets was retained in PFS-b-AGAG (PFS = polyferrocenylsilane) and PFS-g-AGAG conjugates with block and graft architectures, respectively. In the solid state, DSC experiments suggest a phase separation between the peptide and PFS domains. In toluene, PFS-b-AGAG interestingly forms a fibrous network which consists of a core containing the self-assembled antiparallel beta-sheet peptide and a corona of organometallic PFS. The self-assembly of the peptide into antiparallel beta-sheets is the driving force for the fiber formation, whereas PFS prevents uncontrolled lateral aggregation of the fibers. The use of an oligopeptide to self-assemble an otherwise random coiled organometallic polymer may be a useful strategy to enhance nanostructure formation. In the cases described here, the conjugates may be used to create nanopatterned ceramics, and the redox properties of the resulting supramolecular aggregates are of significant interest.     

Interactions between the leucine-zipper motif of cGMP-dependent protein kinase and the C-terminal region of the targeting subunit of myosin light chain phosphatase

Nitric oxide induces vasodilation by elevating the production of cGMP, an activator of cGMP-dependent protein kinase (PKG). PKG subsequently causes smooth muscle relaxation in part via activation of myosin light chain phosphatase (MLCP). To date, the interaction between PKG and the targeting subunit of MLCP (MYPT1) is not fully understood. Earlier studies by one group of workers showed that the binding of PKG to MYPT1 is mediated by the leucine-zipper motifs at the N and C termini, respectively, of the two proteins. Another group, however, reported that binding of PKG to MYPT1 did not require the leucine-zipper motif of MYPT1. In this work we fully characterized the interaction between PKG and MYPT1 using biophysical techniques. For this purpose we constructed a recombinant PKG peptide corresponding to a predicted coiled coil region that contains the leucine-zipper motif. We further constructed various C-terminal MYPT1 peptides bearing various combinations of a predicted coiled coil region, extensions preceding this coiled coil region, and the leucine-zipper motif. Our results show, firstly, that while the leucine-zipper motif at the N terminus of PKG forms a homodimeric coiled coil, the one at the C terminus of MYPT1 is monomeric and non-helical. Secondly, the leucine-zipper motif of PKG binds to that of MYPT1 to form a heterodimer. Thirdly, when the leucine-zipper motif of MYPT1 is absent, the PKG leucine-zipper motif binds to the coiled coil region and upstream segments of MYPT1 via formation of a heterotetramer. These results provide rationalization of some of the findings by others using alternative binding analyses.     

Buried polar interactions and conformational stability in the simian immunodeficiency virus (SIV) gp41 core

For human (HIV) and simian (SIV) immunodeficiency viruses, the gp41 envelope protein undergoes a receptor-activated conformational change from a labile native structure to an energetically more stable fusogenic conformation, which then mediates viral-cell membrane fusion. The core structure of fusion-active gp41 is a six-helix bundle in which three antiparallel carboxyl-terminal helices are packed against an amino-terminal trimeric coiled coil. Here we show that a recombinant model of the SIV gp41 core, designated N36(L6)C34, forms an alpha-helical trimer that exhibits a cooperative two-state folding-unfolding transition. We investigate the importance of buried polar interactions in determining the overall fold of the gp41 core. We have replaced each of four polar amino acids at the heptad a and d positions of the coiled coil in N36(L6)C34 with a representative hydrophobic amino acid, isoleucine. The Q565I, T582I, and T586I variants form six-helix bundle structures that are significantly more stable than that of the wild-type peptide, whereas the Q575I variant misfolds into an insoluble aggregate under physiological conditions. Thus, the buried polar residues within the amino-terminal heptad repeat are important determinants of the structural specificity and stability of the gp41 core. We suggest that these conserved buried polar interactions play a role in governing the conformational state of the gp41 molecule.     

Structure of the Entire Stalk Region of the Dynein Motor Domain

Dyneins are large microtubule-based motor complexes that power a range of cellular processes including the transport of organelles, as well as the beating of cilia and flagella. The motor domain is located within the dynein heavy chain and comprises an N-terminal mechanical linker element, a central ring of six AAA + modules of which four bind or hydrolyze ATP, and a long stalk extending from the AAA + ring with a microtubule-binding domain (MTBD) at its tip. A crucial mechanism underlying the motile activity of cytoskeletal motor proteins is precise coupling between the ATPase and track-binding activities. In dynein, a stalk region consisting of a long (~ 15 nm) antiparallel coiled coil separates these two activities, which must facilitate communication between them. This communication is mediated by a small degree of helix sliding in the coiled coil. However, no high-resolution structure is available of the entire stalk region including the MTBD. Here, we have reported the structure of the entire stalk region of mouse cytoplasmic dynein in a weak microtubule-binding state, which was determined using X-ray crystallography, and have compared it with the dynein motor domain from Dictyostelium discoideum in a strong microtubule-binding state and with a mouse MTBD with its distal portion of the coiled coil fused to seryl-tRNA synthetase from Thermus thermophilus. Our results strongly support the helix-sliding model based on the complete structure of the dynein stalk with a different form of coiled-coil packing. We also propose a plausible mechanism of helix sliding together with further analysis using molecular dynamics simulations. Our results present the importance of conserved proline residues for an elastic motion of stalk coiled coil and imply the manner of change between high-affinity state and low-affinity state of MTBD.     

Structural stability of wild type and mutated alpha-keratin fragments: molecular dynamics and free energy calculations

The objective of this study is to investigate the influence of point mutations on the structural stability of coiled coil fragments of the human hair intermediate filament by molecular dynamics simulations and free energy calculations. Mutations in the helix termination motif of human hair keratin gene hHb6 seem to be connected to the hereditary hair dystrophy Monilethrix. The most common mutations reported are Glu413Lys and Glu413Asp, located at the C-terminal end of the coiled coil 2B rod domain of the IF. According to our simulations, significant conformational changes of the side chains at the mutation and neighboring sites occur due to the Glu413Lys mutation. Furthermore, the differences in electrostatic interactions cause a large change in free energy during transformation of Glu413 to Lys calculated by the thermodynamic integration approach. It is speculated that the structural rearrangement necessary to adapt the interactions in the mutated coiled coil leads to changes in the IF assembly or its stability. The second mutation, Glu413Asp, only leads to a small value of the calculated free energy difference that is within the error limits of the simulations. Thus, it has to be concluded that this mutation does not affect the coiled coil stability.     

Prediction of the stability of coiled coils using molecular dynamics simulations

We have performed 40–80 ns-long molecular dynamics (MD) simulations of the GCN4 leucine zipper and synthetic coiled coils using the GROMOS96 (43a2) and OPLS-AA force fields, with the aim of predicting coiled coil stability. Starting with an initial configuration of two peptides placed in an ideal coiled coil configuration, we find that changing the amino acid sequence modestly or decreasing peptide length can lead to a decrease in the final α-helicity of coiled coils, although for peptides as long or longer than 16 residues, the values of helicity do not decrease to the low values seen in the experimental results of Lumb et al. (Biochemistry. 1994, 33, 7361–7367) or of Su et al. (Biochemistry. 1994, 33, 15501–15510), presumably because the simulations are not long enough. We find, however, that helicity correlates positively with the number of close hydrophobic interactions between the two peptides, showing that stable coiled coils in the simulations are tightly packed. The minimum interhelical distances are 0.50–0.66 nm for charged groups, indicating that favorable charge interactions are also important for the stability of the coiled coil.     

Biochemical and Molecular Dynamic Simulation Analysis of a Weak Coiled Coil Association between Kinesin-II Stalks

Definition

Kinesin-2 refers to the family of motor proteins represented by conserved, heterotrimeric kinesin-II and homodimeric Osm3/Kif17 class of motors.

Background

Kinesin-II, a microtubule-based anterograde motor, is composed of three different conserved subunits, named KLP64D, KLP68D and DmKAP in Drosophila. Although previous reports indicated that coiled coil interaction between the middle segments of two dissimilar motor subunits established the heterodimer, the molecular basis of the association is still unknown.

Methodology/Principal Findings

Here, we present a detailed heterodimeric association model of the KLP64D/68D stalk supported by extensive experimental analysis and molecular dynamic simulations. We find that KLP64D stalk is unstable, but forms a weak coiled coil heteroduplex with the KLP68D stalk when coexpressed in bacteria. Local instabilities, relative affinities between the C-terminal stalk segments, and dynamic long-range interactions along the stalks specify the heterodimerization. Thermal unfolding studies and independent simulations further suggest that interactions between the C-terminal stalk fragments are comparatively stable, whereas the N-terminal stalk reversibly unfolds at ambient temperature.

Conclusions/Significance

Results obtained in this study suggest that coiled coil interaction between the C-terminal stalks of kinesin-II motor subunits is held together through a few hydrophobic and charged interactions. The N-terminal stalk segments are flexible and could uncoil reversibly during a motor walk. This supports the requirement for a flexible coiled coil association between the motor subunits, and its role in motor function needs to be elucidated.     

Presentation of epitopes on genetically engineered peptides and selection of lymphoma-targeting moieties based on epitope biorecognition

A His-tagged coiled coil stem loop peptide with stable secondary structure was designed and biosynthesized. A series of oligopeptides related to the EBV envelope glycoprotein 350/220 N-terminal nonapeptide as potential CD21 receptor-binding epitopes were engineered into the loop region of the peptide scaffold. It was shown that these peptides had a stable alpha-helical coiled coil structure and assumed a monomeric form in PBS. Biorecognition of the epitopes was studied by immobilizing the epitope-containing peptides on complexed Ni2+-containing surfaces through His-Ni2+ chelation and incubating with purified soluble CD21 receptor or CD21+ cells. The results showed that the potential epitopes bound to CD21 and CD21+ cells at different affinities depending on oligopeptide structures. This approach allows for the evaluation of epitope biorecognizabilities and the selection of optimal oligopeptides among sequences for use as targeting moieties in the design of new lymphoma-targeting polymeric drug carriers.