Solution structural characterization of coiled-coil peptide-polymer side-conjugates

Detailed structural characterization of protein-polymer conjugates and understanding of the interactions between covalently attached polymers and biomolecules will build a foundation to design and synthesize hybrid biomaterials. Conjugates based on simple protein structures are ideal model system to achieve these ends. Here we present a systematic structural study of coiled-coil peptide-poly(ethylene glycol) (PEG) side-conjugates in solution, using circular dichroism, dynamic light scattering, and small-angle X-ray scattering, to determine the conformation of conjugated PEG chains. The overall size and shape of side-conjugates were determined using a cylindrical form factor model. Detailed structural information of the covalently attached PEG chains was extracted using a newly developed model where each peptide-PEG conjugate was modeled as a Gaussian chain attached to a cylinder, which was further arranged in a bundle-like configuration of three or four cylinders. The peptide-polymer side-conjugates were found to retain helix bundle structure, with the polymers slightly compressed in comparison with the conformation of free polymers in solution. Such detailed structural characterization of the peptide-polymer conjugates, which elucidates the conformation of conjugated PEG around the peptide and assesses the effect of PEG on peptide structure, will contribute to the rational design of this new family of soft materials.     

Helix stabilization of poly(ethylene glycol)-peptide conjugates

Hybrid polymer-peptide conjugates offer the potential for incorporating biological function into synthetic materials. The secondary structure of short helical peptides, however, frequently becomes less stable when expressed independent of longer protein sequences or covalently linked with a conformationally disordered synthetic polymer. Recently, new amphipathic peptide-poly(ethylene glycol) conjugates were introduced (Shu, J., et al. Biomacromolecules 2008, 9, 2011), which displayed enhanced peptide helicity upon polymer functionalization while retaining tertiary coiled-coil associations. We report here a molecular simulation study of peptide helix stabilization by conjugation with poly(ethylene glycol). The polymer oxygens are shown to favorably interact with the cationic lysine side chains, providing an alternate binding site that protects against disruption of the peptide hydrogen-bonds that stabilize the helical conformation. When the peptide lysine charges are neutralized or poly(ethylene glycol) is conjugated with polyalanine, the polymer exhibits a negligible effect on the secondary structure. We also observe the interactions of poly(ethylene glycol) with the amphipathic peptide lysines tends to segregate the polymer away from the nonpolar face of the helix, suggesting no disruption of the interactions that drive tertiary contacts between helicies.     

Light chain-dependent self-association of dynein intermediate chain

Dynein light chains are bivalent dimers that bind two copies of dynein intermediate chain IC to form a cargo attachment subcomplex. The interaction of light chain LC8 with the natively disordered N-terminal domain of IC induces helix formation at distant IC sites in or near a region predicted to form a coiled-coil. This fostered the hypothesis that LC8 binding promotes IC self-association to form a coiled-coil or other interchain helical structure. However, recent studies show that the predicted coiled-coil sequence partially overlaps the light chain LC7 recognition sequence on IC, raising questions about the apparently contradictory effects of LC8 and LC7. Here, we use NMR and fluorescence quenching to localize IC self-association to residues within the predicted coiled-coil that also correspond to helix 1 of the LC7 recognition sequence. LC8 binding promotes IC self-association of helix 1 from each of two IC chains, whereas LC7 binding reverses self-association by incorporating the same residues into two symmetrical, but distant, helices of the LC7-IC complex. Isothermal titration experiments confirm the distinction of LC8 enhancement of IC self-association and LC7 binding effects. When all three light chains are bound, IC self-association is shifted to another region. Such flexibility in association modes may function in maintaining a stable and versatile light chain-intermediate chain assembly under changing cellular conditions.     

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.     

Intracellular signal-responsive gene carrier for cell-specific gene expression

We designed a peptide-polymer conjugate (CPCCtat) as a novel gene carrier that could control gene expression responding to the intracellular caspase-3 signal. This carrier consists of an uncharged main polymer chain and a cationic peptide side chain, which includes the substrate sequence of caspase-3 and the protein transduction domain sequence of HIV-1 Tat. In the present study, CPCCtat formed a tight complex with DNA through an electrostatic interaction, and in this state the gene expression was totally suppressed. In contrast, the complex disintegrated in the presence of caspase-3 due to cleavage of the cationic portion from CPCCtat. This event led to an activation of gene expression. Our results also indicate that the complex can be delivered into living cells due to the cell-permeable peptide side chain of CPCCtat. This intracellular signal-responsive system with CPCCtat will be useful for the cell-specific gene expression system.     

Construction of a bFGF-tethered extracellular matrix using a coiled-coil helical interaction

A novel method for construction of biomaterials for tissue engineering was developed. Noncovalent associations between extracellular matrix (ECM) and growth factors were achieved by engineering recombinant versions of both proteins that included helical peptides that could form a coiled-coil structure. The helix A peptide, which is capable of forming a coiled-coil helical structure, was fused with a matrix protein that contains a cell-adhesive RGD sequence. The helix B peptide, which is also capable of forming a coiled-coil helical structure, was fused with basic fibroblast growth factor (bFGF). Each protein retained its original activity of promoting cell adhesion and cell proliferation, respectively. These recombinant proteins associated noncovalently through coiled-coil helix formation between helix A and helix B. The resulting complex combined the functions of both proteins, and this method of joining proteins with different functionalities could be used to develop biomaterials for tissue engineering.     

A peptide sequence controls the physical properties of nanoparticles formed by peptide-polymer conjugates that respond to a protein kinase a signal

We previously reported that poly(N-isopropylacrylamide) grafted with Peptide 1 (-GLRRASLG) and poly(ethylene glycol) changed its physical properties in response to an intracellular protein phosphorylation signal, protein kinase A (PKA) (Katayama, Y. et al. (2001) Macromolecules 34, 905). In this study, we investigated the effect of changing peptide structure on the lower critical solution temperature (LCST) of peptide-polymer conjugates, before and after phosphorylation with PKA. For Peptide 2 (Ac-LRRASL-), which has a formal net charge of +2 at physiological pH, the LCST of the conjugate decreased on phosphorylation. In contrast, the LCSTs of the conjugates with Peptide 3 (-ALRRASLE) and Peptide 4 (Ac-DWDALRRASL-), which have neutral net charges, were greatly increased. This suggests that the LCST of the polymer was mainly governed by two factors: the change in hydration around the polymer chain and the interpeptide electrostatic repulsion, resulting from phosphorylation. These polymers have potential for use as drug capsules that respond to cellular conditions.     

Synthesis, characterization, and thermodynamic study of a polyvalent lytic peptide-polymer conjugate as novel anticancer agent

We designed and synthesized a new polyvalent lytic peptide-polymer conjugate as a novel chemotherapeutic agent capable of overcoming multidrug resistance. A hexapeptide (KWKWKW or (KW)?) was designed and conjugated to dextran in multiple copies to afford a polyvalent conjugate. A robust synthesis procedure involving click chemistry and the detailed characterization of the conjugate were reported here. The conjugate Dex-(KW)? exhibited significantly enhanced anticancer potency in vitro by up to 500-fold compared to monomeric (KW)?. The LC?? value was comparable to that of conventional lytic peptides which have more than 20 residues. No hemolytic activity was shown by the conjugates up to 300 μM. Thermodynamic study indicated that the binding of conjugates was predominantly entropy-driven while the binding of free peptides was mainly enthalpy-driven, implying a deeper penetration of conjugate into the core of lipid bilayer. The binding affinity of conjugate to neutral membrane is much higher than that to free peptide (K(conj) ≈ 8822.9 M?1, K(pep) ≈ 1884.7 M?1). In binding to negatively charged membrane, the conjugate surpassed free peptides at high concentrations when the binding of free peptides became saturated. The higher binding capability, attributed to the high local concentration of peptides mounted on a polymer backbone, explains the superior anticancer activity of polyvalent Dex-(KW)?.     

Packing and recognition of protein structural elements: A new approach applied to the 4-helix bundle of myohemerythrin

We present a novel search strategy for determining the optimal packing of protein secondary structure elements. The approach is based on conformational energy optimization using a predetermined set of side chain rotamers and appropriate methods for sampling the conformational space of peptide fragments having fixed backbone geometries. An application to the 4-helix bundle of myohemerythrin is presented. It is shown that the conformations of the amino acid side chains are largely determined at the level of helix pairs and that superposition of these results can be used to construct the full bundle. The final solution obtained, taking into account restrictions due to the lateral amphiphilicity of the helices, differs from the native structure by only a 20° rotation of a single helix. © 1993 Wiley-Liss, Inc.     

A de novo peptide hexamer with a mutable channel

The design of new proteins that expand the repertoire of natural protein structures represents a formidable challenge. Success in this area would increase understanding of protein structure and present new scaffolds that could be exploited in biotechnology and synthetic biology. Here we describe the design, characterization and X-ray crystal structure of a new coiled-coil protein. The de novo sequence forms a stand-alone, parallel, six-helix bundle with a channel running through it. Although lined exclusively by hydrophobic leucine and isoleucine side chains, the 6-? channel is permeable to water. One layer of leucine residues within the channel is mutable, accepting polar aspartic acid and histidine side chains, which leads to subdivision and organization of solvent within the lumen. Moreover, these mutants can be combined to form a stable and unique (Asp-His)(3) heterohexamer. These new structures provide a basis for engineering de novo proteins with new functions.     

The structure of ColE1 rop in solution

Summary The structure of the ColE1 repressor of primer (rop) protein in solution was determined from the proton nuclear magnetic resonance data by a combined use of distance geometry and restrained molecular dynamics calculations. A set of structures was determined with low internal energy and virtually no violations of the experimental distance restraints. Rop forms homodimers: Two helical hairpins are arranged as an antiparallel four helix bundle with a left-handed rope-like twist of the helix axes and with left-handed bundle topology. The very compact packing of the side chains in the helix interfaces of the rop coiled-coil structure may well account for its high stability. Overall, the solution structure is highly similar to the recently determined X-ray structure (Banner, D.W., Kokkinidis, M. and Tsernoglou, D. (1987)J. Mol. Biol.,196, 657–675), although there are minor differences in regions where packing forces appear to influence the crystal structure.Abbreviations rop repressor of primer - NMR nuclear magnetic resonance - NOE nuclear Overhauser enhancement - NOESY NOE spectroscopy - RAN Set Structures generated from random choice of the dihedrai angles - HEL Set Structures generated from random choice of the dihedral angles restricted to ranges allowed for helices - MD molecular dynamics - EM energy minimization - RMSD root-mean-square deviation of atomic positions     

The structure of the C-terminal actin-binding domain of talin

Talin is a large dimeric protein that couples integrins to cytoskeletal actin. Here, we report the structure of the C-terminal actin-binding domain of talin, the core of which is a five-helix bundle linked to a C-terminal helix responsible for dimerisation. The NMR structure of the bundle reveals a conserved surface-exposed hydrophobic patch surrounded by positively charged groups. We have mapped the actin-binding site to this surface and shown that helix 1 on the opposite side of the bundle negatively regulates actin binding. The crystal structure of the dimerisation helix reveals an antiparallel coiled-coil with conserved residues clustered on the solvent-exposed face. Mutagenesis shows that dimerisation is essential for filamentous actin (F-actin) binding and indicates that the dimerisation helix itself contributes to binding. We have used these structures together with small angle X-ray scattering to derive a model of the entire domain. Electron microscopy provides direct evidence for binding of the dimer to F-actin and indicates that it binds to three monomers along the long-pitch helix of the actin filament.     

Packed protein bilayers in the 0.90 A resolution structure of a designed alpha helical bundle.

A 12-residue peptide designed to form an alpha-helix and self-associate into an antiparallel 4-alpha-helical bundle yields a 0.9 A crystal structure revealing unanticipated features. The structure was determined by direct phasing with the "Shake-and-Bake" program, and contains four crystallographically distinct 12-mer peptide molecules plus solvent for a total of 479 atoms. The crystal is formed from nearly ideal alpha-helices hydrogen bonded head-to-tail into columns, which in turn pack side-by-side into sheets spanning the width of the crystal. Within each sheet, the alpha-helices run antiparallel and are closely spaced (9-10 A center-to-center). The sheets are more loosely packed against each other (13-14 A between helix centers). Each sheet is amphiphilic: apolar leucine side chains project from one face, charged lysine and glutamate side chains from the other face. The sheets are stacked with two polar faces opposing and two apolar faces opposing. The result is a periodic biomaterial composed of packed protein bilayers, with alternating polar and apolar interfaces. All of the 30 water molecules in the unit cell lie in the polar interface or between the stacked termini of helices. A section through the sheet reveals that the helices packed at the apolar interface resemble the four-alpha-helical bundle of the design, but the helices overhang parts of the adjacent bundles, and the helix crossing angles are less steep than intended (7-11 degrees rather than 18 degrees).     

Crystal structure of the amino-terminal coiled-coil domain of the APC tumor suppressor

Coiled coils serve as dimerization domains for a wide variety of proteins, including the medically important oligomeric tumor suppressor protein, APC. Mutations in the APC gene are associated with an inherited susceptibility to colon cancer and with approximately 75 % of sporadic colorectal tumors. To define the basis for APC pairing and to explore the anatomy of dimeric coiled coils, we determined the 2.4 A resolution X-ray crystal structure of the N-terminal dimerization domain of APC. The peptide APC-55, encompassing the heptad repeats in APC residues 2-55, primarily forms an alpha-helical, coiled-coil dimer with newly observed core packing features. Correlated asymmetric packing of four core residues in distinct, standard rotamers is associated with a small shift in the helix register. At the C terminus, the helices splay apart and interact with a symmetry-related dimer in the crystal to form a short, anti-parallel, four-helix bundle. N-terminal fraying and C-terminal splaying of the helices, as well as the asymmetry and helix register shift describe unprecedented dynamic excursions of coiled coils. The low stability of APC-55 and divergence from the expected coiled-coil fold support the suggestion that the APC dimerization domain may extend beyond the first 55 residues.     

Empirical and computational design of iron-sulfur cluster proteins

Here, we compare two approaches of protein design. A computational approach was used in the design of the coiled-coil iron-sulfur protein, CCIS, as a four helix bundle binding an iron-sulfur cluster within its hydrophobic core. An empirical approach was used for designing the redox-chain maquette, RCM as a four-helix bundle assembling iron-sulfur clusters within loops and one heme in the middle of its hydrophobic core. We demonstrate that both ways of design yielded the desired proteins in terms of secondary structure and cofactors assembly. Both approaches, however, still have much to improve in predicting conformational changes in the presence of bound cofactors, controlling oligomerization tendency and stabilizing the bound iron-sulfur clusters in the reduced state. Lessons from both ways of design and future directions of development are discussed. This article is part of a Special Issue entitled: Photosynthesis Research for Sustainability: from Natural to Artificial.     

Modulation of the self-assembled structure of biomolecules: coarse grained molecular dynamics simulation

The mechanisms governing the self-assembled structure of biomolecules (single chain and bundle of chains) are studied with an AB copolymer model via the coarse grained molecular dynamics simulations. Non-local hydrophobic interaction is found to play a critical role in the pattern formation of the assembled structure of polymer chains. We show that the polymer structure could be controlled by adjusting the balance between local (short range) and non-local (long range) hydrophobic interaction which are influenced by various factors such as the sequences, chain length, stiffness, confinement, and the topology of polymers. In addition, the competition between the intrachain hydrophobic interaction and interchain hydrophobic interaction determines the structural transition of the chain bundles. This work may provide important insights into the fundamental physics in the structure control and the self-assembly of biomolecules for various practical applications.     

Computational de novo design of a four-helix bundle protein—DND_4HB

The de novo design of proteins is a rigorous test of our understanding of the key determinants of protein structure. The helix bundle is an interesting de novo design model system due to the diverse topologies that can be generated from a few simple α-helices. Previously, noncomputational studies demonstrated that connecting amphipathic helices together with short loops can sometimes generate helix bundle proteins, regardless of the bundle''s exact sequence. However, using such methods, the precise positions of helices and side chains cannot be predetermined. Since protein function depends on exact positioning of residues, we examined if sequence design tools in the program Rosetta could be used to design a four-helix bundle with a predetermined structure. Helix position was specified using a folding procedure that constrained the design model to a defined topology, and iterative rounds of rotamer-based sequence design and backbone refinement were used to identify a low energy sequence for characterization. The designed protein, DND_4HB, unfolds cooperatively (T_m >90°C) and a NMR solution structure shows that it adopts the target helical bundle topology. Helices 2, 3, and 4 agree very closely with the design model (backbone RMSD = 1.11 Å) and >90% of the core side chain χ1 and χ2 angles are correctly predicted. Helix 1 lies in the target groove against the other helices, but is displaced 3 Å along the bundle axis. This result highlights the potential of computational design to create bundles with atomic-level precision, but also points at remaining challenges for achieving specific positioning between amphipathic helices.     

Molecular dynamics simulation of a synthetic ion channel.

A molecular dynamics simulation has been performed on a synthetic membrane-spanning ion channel, consisting of four alpha-helical peptides, each of which is composed of the amino acids leucine (L) and serine (S), with the sequence Ac-(LSLLLSL)3-CONH2. This four-helix bundle has been shown experimentally to act as a proton-conducting channel in a membrane environment. In the present simulation, the channel was initially assembled as a parallel bundle in the octane portion of a phase-separated water/octane system, which provided a membrane-mimetic environment. An explicit reversible multiple-time-step integrator was used to generate a dynamical trajectory, a few nanoseconds in duration for this composite system on a parallel computer, under ambient conditions. After more than 1 ns, the four helices were found to adopt an associated dimer state with twofold symmetry, which evolved into a coiled-coil tetrameric structure with a left-handed twist. In the coiled-coil state, the polar serine side chains interact to form a layered structure with the core of the bundle filled with H2O. The dipoles of these H2O molecules tended to align opposite the net dipole of the peptide bundle. The calculated dipole relaxation function of the pore H2O molecules exhibits two reorientation times. One is approximately 3.2 ps, and the other is approximately 100 times longer. The diffusion coefficient of the pore H2O is about one-third of the bulk H2O value. The total dipole moment and the inertia tensor of the peptide bundle have been calculated and reveal slow (300 ps) collective oscillatory motions. Our results, which are based on a simple united atom force-field model, suggest that the function of this synthetic ion channel is likely inextricably coupled to its dynamical behavior.