Sticky-end assembly of a designed peptide fiber provides insight into protein fibrillogenesis

Coiled-coil motifs provide simple systems for studying molecular self-assembly. We designed two 28-residue peptides to assemble into an extended coiled-coil fiber. Complementary interactions in the core and flanking ion-pairs were used to direct staggered heterodimers. These had "sticky-ends" to promote the formation of long fibers. For comparison, we also synthesized a permuted version of one peptide to associate with the other peptide and form canonical heterodimers with "blunt-ends" that could not associate longitudinally. The assembly of both pairs was monitored in solution using circular dichroism spectroscopy. In each case, mixing the peptides led to increased and concentration-dependent circular dichroism signals at 222 nm, consistent with the desired alpha-helical structures. For the designed fiber-producing peptide mixture, we also observed a linear dichroism effect during flow orientation, indicative of the presence of long fibrous structures. X-ray fiber diffraction of partially aligned samples gave patterns indicative of coiled-coil structure. Furthermore, we used electron microscopy to visualize fiber formation directly. Interestingly, the fibers observed were at least several hundred micrometers long and 20 times thicker than expected for the dimeric coiled-coil design. This additional thickness implied lateral association of the designed structures. We propose that complementary features present in repeating structures of the type we describe promote lateral assembly, and that a similar mechanism may underlie fibrillogenesis in certain natural systems.     

Unraveling double stranded alpha-helical coiled coils: an x-ray diffraction study on hard alpha-keratin fibers

Transformations of proteins secondary and tertiary structures are generally studied in globular proteins in solution. In fibrous proteins, such as hard alpha-keratin, that contain long and well-defined double stranded alpha-helical coiled coil domains, such study can be directly done on the native fibrous tissue. In order to assess the structural behavior of the coiled coil domains under an axial mechanical stress, wide angle x-ray scattering and small angle x-ray scattering experiments have been carried out on stretched horse hair fibers at relative humidity around 30%. Our observations of the three major axial spacings as a function of the applied macroscopic strain have shown two rates. Up to 4% macroscopic strain the coiled coils were slightly distorted but retained their overall conformation. Above 4% the proportion of coiled coil domains progressively decreased. The main and new result of our study is the observation of the transition from alpha-helical coiled coils to disordered chains instead of the alpha-helical coiled coil to beta-sheet transition that occurs in wet fibers.     

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.     

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.     

Extended, relaxed, and condensed conformations of hyaluronan observed by atomic force microscopy

The conformation of the polysaccharide hyaluronan (HA) has been investigated by tapping mode atomic force microscopy in air. HA deposited on a prehydrated mica surface favored an extended conformation, attributed to molecular combing and inhibition of subsequent chain recoil by adhesion to the structured water layer covering the surface. HA deposited on freshly cleaved mica served as a defect in a partially structured water layer, and favored relaxed, weakly helical, coiled conformations. Intramolecularly condensed forms of HA were also observed, ranging from pearl necklace forms to thick rods. The condensation is attributed to weak adhesion to the mica surface, counterion-mediated attractive electrostatic interactions between polyelectrolytes, and hydration effects. Intermolecular association of both extended and condensed forms of HA was observed to result in the formation of networks and twisted fibers, in which the chain direction is not necessarily parallel to the fiber direction. Whereas the relaxed coil and partially condensed conformations of HA are relevant to the native structure of liquid connective tissues, fully condensed rods may be more relevant for HA tethered to a cell surface or intracellular HA, and fibrous forms may be relevant for HA subjected to shear flow in tight intercellular spaces or in protein-HA complexes.     

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.     

Crystal structure of a super leucine zipper,an extended two‐stranded super long coiled coil

Coiled coil is a ubiquitous structural motif in proteins, with two to seven alpha helices coiled together like the strands of a rope, and coiled coil folding and assembly is not completely understood. A GCN4 leucine zipper mutant with four mutations of K3A, D7A, Y17W, and H18N has been designed, and the crystal structure has been determined at 1.6 Å resolution. The peptide monomer shows a helix trunk with short curved N‐ and C‐termini. In the crystal, two monomers cross in 35° and form an X‐shaped dimer, and each X‐shaped dimer is welded into the next one through sticky hydrophobic ends, thus forming an extended two‐stranded, parallel, super long coiled coil rather than a discrete, two‐helix coiled coil of the wild‐type GCN4 leucine zipper. Leucine residues appear at every seventh position in the super long coiled coil, suggesting that it is an extended super leucine zipper. Compared to the wild‐type leucine zipper, the N‐terminus of the mutant has a dramatic conformational change and the C‐terminus has one more residue Glu 32 determined. The mutant X‐shaped dimer has a large crossing angle of 35° instead of 18° in the wild‐type dimer. The results show a novel assembly mode and oligomeric state of coiled coil, and demonstrate that mutations may affect folding and assembly of the overall coiled coil. Analysis of the formation mechanism of the super long coiled coil may help understand and design self‐assembling protein fibers.     

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.     

Engineering of the hydrophobic core of an alpha-helical coiled coil

The amino acid sequence that forms the alpha-helical coiled coil structure has a representative heptad repeat denoted by defgabc, according to their positions. Although the a and d positions are usually occupied by hydrophobic residues, hydrophilic residues at these positions sometimes play important roles in natural proteins. We have manipulated a few amino acids at the a and d positions of a de novo designed trimeric coiled coil to confer new functions to the peptides. The IZ peptide, which has four heptad repeats and forms a parallel triple-stranded coiled coil, has Ile at all of the a and d positions. We show three examples: (1) the substitution of one Ile at either the a or d position with Glu caused the peptide to become pH sensitive; (2) the metal ion induced alpha-helical bundles were formed by substitutions with two His residues at the d and a positions for a medium metal ion, and with one Cys residue at the a position for a soft metal ion; and (3) the AAB-type heterotrimeric alpha-helical bundle formation was accomplished by a combination of Ala and Trp residues at the a positions of different peptide chains. Furthermore, we applied these procedures to prepare an ABC-type heterotrimeric alpha-helical bundle and a metal ion-induced heterotrimeric alpha-helical bundle.     

Developmental stage dependent expression of the endothelial stress fibers and organization of fibronectin fibrils in the aorta of chick embryos

Organizational relationships between endothelial stress fibers and fibronectin fibrils in the developing chick abdominal aorta, from 5th day embryos to 3rd day young chicks, were studied with immunofluorescence and electron microscopy. Stress fibers, axially aligned parallel to the longitudinal cell axis, were expressed in the largely elongated endothelial cells, in embryos older than 8th day of incubation. Fibronectin fibrils in the aortic basal lamina, changed its organizational pattern from the network-like form to the straight bundles arranged parallel to the vessel's longitudinal axis after 9th day of incubation. Such axial alignment was dominant in the matrix beneath the elongated cells containing stress fibers, suggesting the existence of stress fibers may possibly modify the fibronectin's organizational pattern. The vinculin-containing dense plaque, which shaped like as the adhesion plaque in the cultured cells, was located at the ends of or lateral associating sites of stress fibers in embryos older than 8th day stage. The expression of stress fibers, as well as the formation of stress fiber's end plaques, may closely relate to the alignment between the stress fiber and fibronectin fibrils in the extracellular matrix.     

The effect of N-terminal acetylation on the structure of an N-terminal tropomyosin peptide and alpha alpha-tropomyosin.

We have used a synthetic peptide consisting of the first 30 residues of striated muscle alpha-tropomyosin, with GlyCys added to the C-terminus, to investigate the effect of N-terminal acetylation on the conformation and stability of the N-terminal domain of the coiled-coil protein. In aqueous buffers at low ionic strength, the reduced, unacetylated 32mer had a very low alpha-helical content (approximately 20%) that was only slightly increased by disulfide crosslinking or N-terminal acetylation. Addition of salt (> 1 M) greatly increased the helical content of the peptide. The CD spectrum, the cooperativity of folding of the peptide, and sedimentation equilibrium ultracentrifugation studies showed that it formed a 2-chained coiled coil at high ionic strength. Disulfide crosslinking and N-terminal acetylation both greatly stabilized the coiled-coil alpha-helical conformation in high salt. Addition of ethanol or trifluoroethanol to solutions of the peptide also increased its alpha-helical content. However, the CD spectra and unfolding behavior of the peptide showed no evidence of coiled-coil formation. In the presence of the organic solvents, N-terminal acetylation had very little effect on the conformation or stability of the peptide. Our results indicate that N-terminal acetylation stabilizes coiled-coil formation in the peptide. The effect cannot be explained by interactions with the "helix-dipole" because the stabilization is observed at very high salt concentrations and is independent of pH. In contrast to the results with the peptide, N-terminal acetylation has only small effects on the overall stability of tropomyosin.     

Raman spectroscopy of cytoplasmic muscle fiber proteins. Orientational order.

The polarized Raman spectra of glycerinated and intact single muscle fibers of the giant barnacle were obtained. These spectra show that the conformation-sensitive amide I, amide III, and C-C stretching vibrations give Raman bands that are stronger when the electric field of both the incident and scattered radiation is parallel to the fiber axis (Izz). The detailed analysis of the amide I band by curve fitting shows that approximately 50% of the alpha-helical segments of the contractile proteins are oriented along the fiber axis, which is in good agreement with the conformation and composition of muscle fiber proteins. Difference Raman spectroscopy was also used to highlight the Raman bands attributed to the oriented segments of the alpha-helical proteins. The difference spectrum, which is very similar to the spectrum of tropomyosin, displays amide I and amide III bands at 1,645 and 1,310 cm-1, respectively, the bandwidth of the amide I line being characteristic of a highly alpha-helical biopolymer with a small dispersion of dihedral angles. A small dichroic effect was also observed for the band due to the CH2 bending mode at 1,450 cm-1 and on the 1,340 cm-1 band. In the C-C stretching mode region, two bands were detected at 902 and 938 cm-1 and are both assigned to the alpha-helical conformation.     

Review: conformation and folding of novel beta-structural elements in viral fiber proteins: the triple beta-spiral and triple beta-helix

Apart from alpha-helical coiled coils and the collagen triple helices, fibrous proteins can contain beta-structure in various conformations. Elongated enzymes such as pectate lyase and the bacteriophage P22 tailspike protein contain single-stranded beta-helices. Virus and bacteriophage fibers, which are often trimeric, have been shown to contain novel triple-stranded beta-structures such as the triple beta-spiral and the triple beta-helix. The conformation and folding of viral fibers containing beta-structure are discussed.     

Fibers of tau fragments, but not full length tau, exhibit a cross beta-structure: implications for the formation of paired helical filaments

We have used X-ray fiber diffraction to probe the structure of fibers of tau and tau fragments. Fibers of fragments from the microtubule binding domain had a cross beta-structure that closely resembles that reported both for neurofibrillary tangles found in Alzheimer's disease brain and for fibrous lesions from other protein folding diseases. In contrast, fibers of full-length tau had a different, more complex structure. Despite major differences at the molecular level, all fiber types exhibited very similar morphology by electron microscopy. These results have a number of implications for understanding the etiology of Alzheimer's and other tauopathic diseases. The morphology of the peptide fibers suggests that the region in tau corresponding to the peptides plays a critical role in the nucleation of fiber assembly. The dramatically different structure of the full length tau fibers suggests that some region in tau has enough inherent structure to interfere with the formation of cross beta-fibers. Additionally, the similar appearance by electron microscopy of fibrils with varying molecular structure suggests that different molecular arrangements may exist in other samples of fibers formed from tau.     

Motions of tropomyosin. Crystal as metaphor.

Movements of tropomyosin play an essential role in muscle regulation. This fibrous protein is a two-chain alpha-helical coiled coil that bonds head to tail to form cables wound in the two long grooves of the actin helix. The regulatory switch consists of tropomyosin and a "globular" Ca2+-sensitive protein complex called troponin. The structure of the tropomyosin filaments has now been determined by x-ray crystallography to approximately 15 A resolution. The complete sequence of alpha-tropomyosin is known; by using mercury markers on the cysteine residues the ends of the molecules in the filaments have been identified. Details of the coiled-coil structure have also been visualized by refinement of models against the diffraction data. The average pitch of the coiled coil is approximately 137 A, so that each tropomyosin molecule can make similar contacts with seven actin monomers. The electron density map also indicates that departures from the alpha-helical coiled coil occur in a few localized regions of the molecule, especially at the overlapping ends. Motions of tropomyosin in the crystal lattice are displaced by the character of the Bragg reflections and the strong diffuse scatter. These effects depend markedly on temperature. It appears that the molecular filaments fluctuate freely in a direction perpendicular to their axes. Moreover, the C-terminal half of the molecule "unfolds" to some degree at less than physiological temperatures. Crystallographic results on co-crystals of tropomyosin and a component of troponin (TnT) suggest that this subunit consists of structurally distinct domains, so that the troponin complex is not in fact simply "globular". The interactions of the extended alpha-helical region of TnT may "stiffen" tropomyosin and influence its motions. We picture the tropomyosin/troponin switch in muscle as a restless cable, perpetually making and breaking bonds as it vibrates on the thin filament. These movements of tropomyosin probably depend on two aspects of its design: the regular pattern of coiled-coil linkages with actin; and the aperiodic features that allow flexibility and motion.     

An alanine-zipper structure determined by long range intermolecular interactions

A major challenge in protein folding is to identify and quantify specific structural determinants that allow native proteins to acquire their unique folded structures. Here we report the engineering of a 52-residue protein (Ala-14) that contains exclusively alanine residues at the hydrophobic a and d positions of a natural heptad-repeat sequence. Ala-14 is unfolded under normal solution conditions yet forms a parallel three-stranded alpha-helical coiled coil in crystals. Ala-14 trimers in the solid state associate with each other through the pairing of polar side chains and formation of an extended network of water-mediated hydrogen bonds. In contrast to the classical view that local intramolecular tertiary interactions dictate the three-dimensional structure of small single-domain proteins, Ala-14 shows that long range intermolecular interactions can be essential in determining the metastable alanine-zipper structure. A similar interplay between short range local and longer range global forces may underlie the conformational properties of the growing class of natively unstructured proteins in biological processes.     

Plectin: a cytolinker by design

Plectin is a cytoskeletal protein of >500 kDa that forms dumbbell-shaped homodimers comprising a central parallel alpha-helical coiled coil rod domain flanked by globular domains, thus providing a molecular backbone ideally suited to mediate the protein's interactions with an array of other cytoskeletal elements. Plectin self-associates and interacts with actin and intermediate filament cytoskeleton networks at opposite ends, and it binds at both ends to the hemidesmosomal transmembrane protein integrin beta-4, and likely to other junctional proteins. The central coiled coil rod domain can form bridges over long stretches and serves as a flexible linker between the structurally diverse N-terminal domain and the highly conserved C-terminal domain. Plectin is also a target of p34cdc2 kinase that regulates its dissociation from intermediate filaments during mitosis.     

Visualization of G1 chromosomes: a folded, twisted, supercoiled chromonema model of interphase chromatid structure

We have used light microscopy and serial thin-section electron microscopy to visualize intermediates of chromosome decondensation during G1 progression in synchronized CHO cells. In early G1, tightly coiled 100-130-nm "chromonema" fibers are visualized within partially decondensed chromatin masses. Progression from early to middle G1 is accompanied by a progressive uncoiling and straightening of these chromonema fibers. Further decondensation in later G1 and early S phase results in predominantly 60-80-nm chromonema fibers that can be traced up to 2-3 microns in length as discrete fibers. Abrupt transitions in diameter from 100-130 to 60-80 nm along individual fibers are suggestive of coiling of the 60-80-nm chromonema fibers to form the thicker 100-130-nm chromonema fiber. Local unfolding of these chromonema fibers, corresponding to DNA regions tens to hundreds of kilobases in length, reveal more loosely folded and extended 30-nm chromatin fibers. Kinks and supercoils appear as prominent features at all observed levels of folding. These results are inconsistent with prevailing models of chromosome structure and, instead, suggest a folded chromonema model of chromosome structure.