Design, folding, and activities of metal-assembled coiled coil proteins

Metal ions serve many purposes in natural proteins, from the stabilization of tertiary structure to the direction of protein folding to crucial roles in electron transfer and catalysis. There is considerable interest in creating metal binding sites in designed proteins to understand the structural role of metal ions and to design new metalloproteins with useful functions. The de novo design of metalloproteins and the role of metals in the folding of designed proteins are reviewed here, with particular focus on the design, folding, and activities of the [M(bpy-peptide)(3)](2+) structure. This maquette is constructed by the covalent attachment of 2,2'-bipyridine to the N-termini of amphiphilic peptides, and it is assembled into a folded trimeric coiled coil by the addition of a six-coordinate transition metal ion and the resulting hydrophobic collapse of the peptides. The [M(bpy-peptide)(3)](2+) structure has been employed in diverse applications, ranging from electron transfer pathway studies to the study of optimal hydrophobic packing in a virtual library to the construction of receptors and biosensors.     

Assessing the integrity of designed homomeric parallel three-stranded coiled coils in the presence of metal ions

De novo design of alpha-helical peptides that self-assemble to form helical coiled coils is a powerful tool for studying molecular recognition between peptides/proteins and determining the fundamental forces involved in their folding and structure. These amphipathic helices assemble in aqueous solution to generate the final coiled coil motif, with the hydrophobic residues in the interior and the polar/hydrophilic groups on the exterior. Considerable effort has been devoted to investigate the forces that determine the overall stability and final three-dimensional structure of the coiled coils. One of the major challenges in coiled coil design is the achievement of specificity in terms of the oligomeric state, with respect to number (two, three, four, or higher), nature (homomers vs heteromers), and strand orientation (parallel vs antiparallel). As seen in nature, metal ions play an important role in this self-organization process, and the overall structure of metalloproteins is primarily the result of two driving forces: the metal coordination preference and the fold of the polypeptide backbone. Previous work in our group has shown that metal ions such as As(III) and Hg(II) can be used to enforce different aggregation states in the Cys derivatives of the designed homotrimeric coiled-coil TRI family [Ac-G(LKALEEK)4G-CONH2]. We are now interested in studying the interplay between the metal ion and peptide preferences in controlling the specificity and relative orientation of the alpha-helices in coiled coils. For this objective, two derivatives of the TRI family, TRi L2WL9C and TRi L2WL23C, have been synthesized. Along with those two peptides, two derivatives of Coil-Ser, CSL9C and CSL19C (CS = Ac-EWEALEKKLAALESKLQALEKKLEALEHG-CONH2), a similar de novo designed three-stranded coiled coil that has the potential to form antiparallel coiled coils, have also been used. Circular dichroism, UV-vis, and 199Hg and 113Cd NMR spectroscopy results reveal that the addition of Hg(II) and Cd(II) to the different mixtures of these peptides forms preferentially homotrimeric coiled coils, over a statistical population of heterotrimeric parallel and antiparallel coiled coils.     

Design of thiolate rich metal binding sites within a peptidic framework

A de novo protein design strategy provides a powerful tool to elucidate how heavy metals interact with proteins.Cysteine derivatives of the TRI peptide family (Ac-G(LKALEEK)4G-NH2) have been shown to bind heavy metals in an unusual trigonal geometry. Our present objective was to design binding sites in R-helical scaffolds that are able to form higher coordination number complexes with Cd(II) and Hg(II). Herein, we evaluate the binding of Cd(II) and Hg(II) to double cysteine substituted TRI peptides lacking intervening leucines between sulfurs in the heptads. We compare a -Cysd-X-X-X-Cysa- binding motif found in TRIL12CL16C to the more common -Cysa-X-X-Cysd- sequence of native proteins found in TRIL9CL12C. Compared to TRI, these substitutions destabilize the helical aggregates,leading to mixtures of two- and three-stranded bundles. The three-stranded coiled coils are stabilized by the addition of metals. TRIL9CL12C forms distorted tetrahedral complexes with both Cd(II) and Hg(II), as supported by UV-vis,CD, 113Cd NMR, 199Hg NMR and 111mCd PAC spectroscopy. Additionally, these signatures are very similar to those found for heavy metal substituted rubredoxin. These results suggest that in terms of Hg(II) binding, TRIL9CL12Ccan be considered as a good mimic of the metallochaperone HAH1, that has previously been shown to form protein dimers. TRIL12CL16C has limited ability to generate homoleptic tetrahedral complexes (Cd(SR)42-). These type of complexes were identified only for Hg(II). However, the spectroscopic signatures suggest a different geometry around the metal ion, demonstrating that effective metal sequestration into the hydrophobic interior of the bundle requires more than simply adding two sulfur residues in adjacent layers of the peptide core. Thus, proper design of metal binding sites must also consider the orientation of cysteine sidechains in a vs d positions of the heptads.     

Making or Breaking Metal-Dependent Catalytic Activity: The Role of Stammers in Designed Three-Stranded Coiled Coils

While many life-critical reactions would be infeasibly slow without metal cofactors, a detailed understanding of how protein structure can influence catalytic activity remains elusive. Using de novo designed three-stranded coiled coils ( TRI and Grand peptides formed using a heptad repeat approach), we examine how the insertion of a three residue discontinuity, known as a stammer insert, directly adjacent to a (His)₃ metal binding site alters catalytic activity. The stammer, which locally alters the twist of the helix, significantly increases copper-catalyzed nitrite reductase activity (CuNiR). In contrast, the well-established zinc-catalyzed carbonic anhydrase activity (p-nitrophenyl acetate, pNPA) is effectively ablated. This study illustrates how the perturbation of the protein sequence using non-coordinating and non-acid base residues in the helical core can perturb metalloenzyme activity through the simple expedient of modifying the helical pitch adjacent to the catalytic center.     

The application of (199)Hg NMR and (199m)Hg perturbed angular correlation (PAC) spectroscopy to define the biological chemistry of Hg(II): a case study with designed two- and three-stranded coiled coils

The use of de novo designed peptides is a powerful strategy to elucidate Hg(II)-protein interactions and to gain insight into the chemistry of Hg(II) in biological systems. Cysteine derivatives of the designed alpha-helical peptides of the TRI family [Ac-G-(L(a)K(b)A(c)L(d)E(e)E(f)K(g))(4)-G-NH(2)] bind Hg(II) at high pH values and at peptide/Hg(II) ratios of 3:1 with an unusual trigonal thiolate coordination mode. The resulting Hg(II) complexes are good water-soluble models for Hg(II) binding to the protein MerR. We have carried out a parallel study using (199)Hg NMR and (199m)Hg perturbed angular correlation (PAC) spectroscopy to characterize the distinct species that are generated under different pH conditions and peptide TRI L9C/Hg(II) ratios. These studies prove for the first time the formation of [Hg{(TRI L9C)(2)-(TRI L9C-H)}], a dithiolate-Hg(II) complex in the hydrophobic interior of the three-stranded coiled coil (TRI L9C)(3). (199)Hg NMR and (199m)Hg PAC data demonstrate that this dithiolate-Hg(II) complex is different from the dithiolate [Hg(TRI L9C)(2)], and that the presence of third alpha-helix, containing a protonated cysteine, breaks the symmetry of the coordination environment present in the complex [Hg(TRI L9C)(2)]. As the pH is raised, the deprotonation of this third cysteine generates the trigonal thiolate-Hg(II) complex Hg(TRI L9C)(3)(-) on a timescale that is slower than the NMR timescale (0.01-10 ms). The formation of the species [Hg{(TRI L9C)(2)(TRI L9C-H)}] is the result of a compromise between the high affinity of Hg(II) to form dithiolate complexes and the preference of the peptide to form a three-stranded coiled coil.     

Role of cofactors in folding of the blue-copper protein azurin

Many proteins in living cells coordinate cofactors, such as metal ions, to attain their activity. Since the cofactors in such cases often can interact with their corresponding unfolded polypeptides in vitro, it is important to unravel how cofactors modulate protein folding. In this review, I will discuss the role of cofactors in folding of the blue-copper protein Pseudomonas aeruginosa azurin. In the case of both copper (Cu(II) and Cu(I)) and zinc (Zn(II)), the metal can bind to unfolded azurin. The residues involved in copper (Cu(II) and Cu(I)) coordination in the unfolded state have been identified as Cys112, His117, and Met121. The affinities of Cu(II), Cu(I), and Zn(II) are all higher for the folded than for the unfolded azurin polypeptide, resulting in metal stabilization of the native state as compared to the stability of apo-azurin. Cu(II), Zn(II), and several apo forms of azurin all fold in two-state kinetic reactions with roughly identical polypeptide-folding speeds. This suggests that the native-state beta-barrel topology, not cofactor interactions or thermodynamic stability, determines azurin's folding barrier. Nonetheless, copper binds much more rapidly (i.e., 4 orders of magnitude) to unfolded azurin than to folded azurin. Therefore, the fastest route to functional azurin is through copper binding before polypeptide folding; this sequence of events may be the relevant biological pathway.     

Comparison of the binding of cadmium(II), mercury(II), and arsenic(III) to the de novo designed peptides TRI L12C and TRI L16C

Designed alpha-helical peptides of the TRI family with a general sequence Ac-G(LKALEEK)(4)G-CONH(2) were used as model systems for the study of metal-protein interactions. Variants containing cysteine residues in positions 12 (TRI L12C) and 16 (TRI L16C) were used for the metal binding studies. Cd(II) binding was investigated, and the results were compared with previous and current work on Hg(II) and As(III) binding. The metal peptide assemblies were studied with the use of UV, CD, EXAFS, (113)Cd NMR, and (111m)Cd perturbed angular correlation spectroscopy. The metalated peptide aggregates exhibited pH-dependent behavior. At high pH values, Cd(II) was bound to the three sulfurs of the three-stranded alpha-helical coiled coils. A mixture of two species was observed, including Cd(II) in a trigonal planar geometry. The complexes have UV bands at 231 nm (20 600 M(-1) cm(-1)) for TRI L12C and 232 nm (22 600 M(-1) cm(-1)) for TRI L16C, an average Cd-S bond length of 2.49 A for both cases, and a (113)Cd NMR chemical shift at 619 ppm (Cd(II)(TRI L12C)(3)(-)) or 625 ppm (Cd(II)(TRI-L16C)(3)(-)). Nuclear quadrupole interactions show that two different Cd species are present for both peptides. One species with omega(0) = 0.45 rad/ns and low eta is attributed to a trigonal planar Cd-(Cys)(3) site. The other, with a smaller omega(0), is attributed to a four-coordinate Cd(Cys)(3)(H(2)O) species. At low pH, no metal binding was observed. Hg(II) binding to TRI L12C was also found to be pH dependent, and a 3:1 sulfur-to-mercury(II) species was observed at pH 9.4. These metal peptide complexes provide insight into heavy metal binding and metalloregulatory proteins such as MerR or CadC.     

Two-metal ion, Ni(II) and Cu(II), binding alpha-helical coiled coil peptide

Metalloproteins are an attractive target for de novo design. Usually, natural proteins incorporate two or more (hetero- or homo-) metal ions into their frameworks to perform their functions, but the design of multiple metal-binding sites is usually difficult to achieve. Here, we undertook the de novo engineering of heterometal-binding sites, Ni(II) and Cu(II), into a designed coiled coil structure based on an isoleucine zipper (IZ) peptide. Previously, we described two peptides, IZ-3adH and IZ-3aH. The former has two His residues and forms a triple-stranded coiled coil after binding Ni(II), Zn(II), or Cu(II). The latter has one His residue, which allowed binding with Cu(II) and Zn(II), but not with Ni(II). On the basis of these properties, we newly designed IZ(5)-2a3adH as a heterometal-binding peptide. This peptide can bind Cu(II) and Ni(II) simultaneously in the hydrophobic core of the triple-stranded coiled coil. The first metal ion binding induced the folding of the peptide into the triple-stranded coiled coil, thereby promoting the second metal ion binding. This is the first example of a peptide that can bind two different metal ions. This construction should provide valuable insights for the de novo design of metalloproteins.     

全新设计蛋白质的折叠机制

蛋白质全新设计和折叠研究是从两个不同的方向来理解蛋白质序列-结构-功能关系这一结构生物学重要问题. 蛋白质全新设计取得的成功实例一定程度上检验了人们对蛋白质结构和相互作用理解的准确性, 但它们中多数所表现的不同于天然蛋白质的折叠动力学特征也表明, 要达到最终的功能化实现目标还面临着不少的挑战. 本文综述了蛋白质全新设计的发展过程及现状, 蛋白质折叠研究在实验、理论及模拟方面的研究进展, 以及全新设计蛋白质的折叠机制的研究现状. 阐述了深入了解全新设计蛋白质与天然蛋白质折叠机制的不同, 可以为进一步有效地合理化设计蛋白质提供有益的参考.     

Length dependent folding kinetics of phenylacetylene oligomers: structural characterization of a kinetic trap

Using simulation to study the folding kinetics of 20-mer poly-phenylacetylene (pPA) oligomers, we find a long time scale trapped kinetic phase in the cumulative folding time distribution. This is demonstrated using molecular dynamics to simulate an ensemble of over 100 folding trajectories. The simulation data are fit to a four-state kinetic model which includes the typical folded and unfolded states, along with an intermediate state, and most surprisingly, a kinetically trapped state. Topologically diverse conformations reminiscent of alpha helices, beta turns, and sheets in proteins are observed, along with unique structures in the form of knots. The nonhelical conformations are implicated, on the basis of structural correlations to kinetic parameters, to contribute to the trapped kinetic behavior. The strong solvophobic forces which mediate the folding process and produce a stable helical folded state also serve to overstabilize the nonhelical conformations, ultimately trapping them. From our simulations, the folding time is predicted to be on the order of 2.5-12.5 mus in the presence of the trapped kinetic phase. The folding mechanism for these 20-mer chains is compared with the previously reported folding mechanism for the pPA 12-mer chains. A linear scaling relationship between the chain length and the mean first passage time is predicted in the absence of the trapped kinetic phase. We discuss the major implications of this discovery in the design of self-assembling nanostructures.     

Site-selective metal binding by designed alpha-helical peptides

It is known that the designed alpha-helical peptide family TRI [(Ac-G(LKALEEK)4G-CONH2)], containing single site substitution of a cysteine for a leucine, is capable of binding Cd(II) within a three-stranded coiled coil. The binding affinity of cadmium is dependent upon the site of substitution, with cysteine incorporated at the a site leading to cadmium complexes of higher affinity than when a d site was modified. In this work we have examined whether this differential binding affinity can be expressed in a di-cysteine-substituted peptide in order to develop site specificity within a designed system. The peptide TRI L9CL19C was used to determine whether significant differences in binding affinities at nearly proximal sites could be achieved in a short designed peptide. On the basis of 113Cd, 1H NMR, and circular dichroic spectroscopies, we have shown that 1 equiv of Cd(II) binds exclusively at the a site. Only after that position is filled does the second site become populated. Thus, the TRI system represents the first example where stoichiometrically equivalent peptides with different sequences form the framework for designing molecular assemblies that show site-specific ion recognition. We propose that the distinct metal affinities are due to the cysteine conformers at different substitution points along the peptide. Furthermore, we have shown that site selectivity in biomolecules can be encoded into relatively short peptides with helical sequences and, therefore, do not necessarily require the extensive protein scaffolds found in natural systems.     

Two-state folding observed in individual protein molecules

The folding dynamics of small proteins are often described in terms of a simple two-state kinetic model. Within this notion, the behavior of individual molecules is expected to be stochastic, with a protein molecule residing in either the unfolded or the folded state for extended periods of time, with intermittent rapid jumps across the free energy barrier. However, a direct observation of this bistable behavior has not been made to date. Rather, previous reports of folding trajectories of individual proteins have shown an unexpected degree of complexity. This raises the question whether the simple kinetic properties derived from classical experiments on large ensembles of molecules are reflected in the folding paths taken by individual proteins. Here we report single-molecule folding/unfolding trajectories observed by fluorescence resonance energy transfer for a protein that meets all criteria of a two state-system. The trajectories, measured on molecules immobilized in lipid vesicles, demonstrate the anticipated bistable behavior, with steplike transitions between folded and unfolded conformations. They further allow us to put an upper bound on the barrier crossing time.     

Influence of Cd2+, Hg2+ and Pb2+ on (+)-catechin binding to bovine serum albumin studied by fluorescence spectroscopic methods

The effect of heavy metal ions, Cd(2+), Hg(2+) and Pb(2+) on (+)-catechin binding to bovine serum albumin (BSA) has been investigated by spectroscopic methods. The results indicated that the presence of heavy metal ions significantly affected the binding modes and binding affinities of (+)-catechin to BSA, and the effects depend on the types of heavy metal ion. One binding mode was found for (+)-catechin with and without Cd(2+), while two binding modes - a weaker one at low concentration and a stronger one at high concentration were found for (+)-catechin in the presence of Hg(2+) and Pb(2+). The presence of Cd(2+) decreased the binding affinities of (+)-catechin for BSA by 20.5%. The presence of Hg(2+) and Pb(2+) decreased the binding affinity of (+)-catechin for BSA by 8.9% and 26.7% in lower concentration, respectively, and increased the binding affinity of (+)-catechin for BSA by 5.2% and 9.2% in higher concentration, respectively. The changed binding affinity and binding distance of (+)-catechin for BSA in the presence of Cd(2+), Hg(2+) and Pb(2+) were mainly because of the conformational change of BSA induced by heavy metal ions. However, the quenching mechanism for (+)-catechin to BSA was based on static quenching combined with non-radiative energy transfer irrespective of the absence or presence of heavy metal ions.     

Direct monitoring of metal ion transfer between two trafficking proteins

To avoid the toxic effects of both essential and nonessential metal ions, cells elaborate a variety of metal ion trafficking proteins that regulate metal ion mobility. While structures of several trafficking proteins have been determined, kinetic characterization of metal ion transfer between cognate protein partners and the factors controlling transfer has lagged behind, in part due to a limitation on methods to monitor the rapid transfer. In this Communication we report studies on the kinetics of Hg2+ transfer between separately expressed components of the flavoenzyme mercuric ion reductase (MerA) that take advantage of the sensitivity of the flavin fluorescence to the charge state of a cysteine thiol in the Hg2+ binding pathway. The thiolate form of C558 in the Tn501 MerA partially quenches the fluorescence of the oxidized enzyme. Protonation or binding of Hg2+ to the thiolate increases the fluorescence, providing a sensitive probe for kinetic analysis of the Hg2+ binding reaction. The kinetics of Hg2+ transfer in both directions between the cysteine pair of the separately expressed N-terminal domain and the C-terminal cysteines (C558, C559) of the catalytic core are presented, along with a model describing the overall process.     

Stability of cyclic beta-hairpins: asymmetric contributions from side chains of a hydrogen-bonded cross-strand residue pair

Amino acid structural propensities measured in "host-guest" model studies are often used in protein structure prediction or to choose appropriate residues in de novo protein design. While this concept has proven useful for helical structures, it is more difficult to apply successfully to beta-sheets. We have developed a cyclic beta-hairpin scaffold as a host for measurement of individual residue contributions to hairpin structural stability. Previously, we have characterized substitutions in non-backbone-hydrogen-bonded strand sites; relative stability differences measured in the cyclic host are highly predictive of changes in folding free energy for linear beta-hairpin peptides. Here, we examine the hydrogen-bonded strand positions of our host. Surprisingly, we find a large favorable contribution to stability from a valine (or isoleucine) substitution immediately preceding the C-terminal cysteine of the host peptide, but not at the cross-strand position of the host or in either strand of a folded linear beta-hairpin (trpzip peptide). Further substitutions in the peptides and NMR structural analysis indicate that the stabilizing effect of valine is general for CX(8)C cyclic hairpins and cannot be explained by particular side-chain-side-chain interactions. Instead, a localized decrease in twist of the peptide backbone on the N-terminal side of the cysteine allows the valine side chain to adopt a unique conformation that decreases the solvent accessibility of the peptide backbone. The conformation differs from the highly twisted (coiled) conformation of the trpzip hairpins and is more typical of conformations present in multistranded beta-sheets. This unexpected structural fine-tuning may explain why cyclic hairpins selected from phage-displayed libraries often have valine in the same position, preceding the C-terminal cysteine. It also emphasizes the diversity of structures accessible to beta-strands and the importance of considering not only "beta-propensity", but also hydrogen-bonding pattern and strand twist, when designing beta structures. Finally, we observe correlated, cooperative stabilization from side-chain substitutions on opposite faces of the hairpin. This suggests that cooperative folding in beta-hairpins and other small beta-structures is driven by cooperative strand-strand association.     

Intrinsic Ca2+ affinities of peptides: Application of the kinetic method to analogs of calcium-binding site III of rabbit skeletal troponin C

We extended the kinetic method to determine the intrinsic affinities of nonvolatile organic molecules with divalent metal ions and then applied the amended method to determine the calcium affinities of peptide analogs of the calcium-binding site III of rabbit skeletal troponin C. Metal-bis(peptide) complexes of the composition ([H2Pi + H2Pii] - H + Ca)+, where H2P is a neutral peptide, were introduced into the gas phase by fast atom bombardment. The extended kinetic method recognizes that the dissociation characteristics of a singly charged, bis(peptide) complexes of divalent metal ions are determined by not only the metal-ion affinity but also the proton affinities of the neutral and deprotonated peptides. The modified method requires one to measure the relative abundances of [H2P - H + Ca]+, [H2P + H]+, and [H2P - H]- ions that form upon collisional activation of mixed peptide/metal complexes, proton-bound peptide dimers, and deprotonated peptide dimers, respectively. We found, by using the modified method, that the set of peptides has a different affinity order than that in solution. Peptides with one aspartic acid have a higher intrinsic Ca2+ affinity than those with two aspartates. The location of the aspartic acid (Asp) residues at various positions also affects the Ca2+ affinity. Those peptides with one Asp in the middle of the chain have higher Ca2+ affinities than those with Asp on the end because the former peptides offer greater polarizability to stabilize the charge. Peptides with two Asp's located in close proximity have higher intrinsic calcium affinities than those with aspartates positioned further apart.     

Folding dynamics of Trp-cage in the presence of chemical interference and macromolecular crowding. I

Proteins fold and function in the crowded environment of the cell's interior. In the recent years it has been well established that the so-called "macromolecular crowding" effect enhances the folding stability of proteins by destabilizing their unfolded states for selected proteins. On the other hand, chemical and thermal denaturation is often used in experiments as a tool to destabilize a protein by populating the unfolded states when probing its folding landscape and thermodynamic properties. However, little is known about the complicated effects of these synergistic perturbations acting on the kinetic properties of proteins, particularly when large structural fluctuations, such as protein folding, have been involved. In this study, we have first investigated the folding mechanism of Trp-cage dependent on urea concentration by coarse-grained molecular simulations where the impact of urea is implemented into an energy function of the side chain and/or backbone interactions derived from the all-atomistic molecular dynamics simulations with urea through a Boltzmann inversion method. In urea solution, the folding rates of a model miniprotein Trp-cage decrease and the folded state slightly swells due to a lack of contact formation between side chains at the terminal regions. In addition, the equilibrium m-values of Trp-cage from the computer simulations are in agreement with experimental measurements. We have further investigated the combined effects of urea denaturation and macromolecular crowding on Trp-cage's folding mechanism where crowding agents are modeled as hard-spheres. The enhancement of folding rates of Trp-cage is most pronounced by macromolecular crowding effect when the extended conformations of Trp-cast dominate at high urea concentration. Our study makes quantitatively testable predictions on protein folding dynamics in a complex environment involving both chemical denaturation and macromolecular crowding effects.     

Determining the Mg2+ stoichiometry for folding an RNA metal ion core

The folding and catalytic function of RNA molecules depend on their interactions with divalent metal ions, such as magnesium. As with every molecular process, the most basic knowledge required for understanding the close relationship of an RNA with its metal ions is the stoichiometry of the interaction. Unfortunately, inventories of the numbers of divalent ions associated with unfolded and folded RNA states have been unattainable. A common approach has been to interpret Hill coefficients fit to folding equilibria as the number of metal ions bound upon folding. However, this approach is vitiated by the presence of diffusely associated divalent ions in a dynamic ion atmosphere and by the likelihood of multiple transitions along a folding pathway. We demonstrate that the use of molar concentrations of background monovalent salt can alleviate these complications. These simplifying solution conditions allow a precise determination of the stoichiometry of the magnesium ions involved in folding the metal ion core of the P4-P6 domain of the Tetrahymena group I ribozyme. Hill analysis of hydroxyl radical footprinting data suggests that the P4-P6 RNA core folds cooperatively upon the association of two metal ions. This unexpectedly small stoichiometry is strongly supported by counting magnesium ions associated with the P4-P6 RNA via fluorescence titration and atomic emission spectroscopy. By pinpointing the metal ion stoichiometry, these measurements provide a critical but previously missing step in the thermodynamic dissection of the coupling between metal ion binding and RNA folding.     

Membrane binding and structure of de novo designed alpha-helical cationic coiled-coil-forming peptides.

We introduce a de novo designed peptide model system that enables the systematic study of 1) the role of a membrane environment in coiled-coil peptide folding, 2) the impact of different domains of an alpha-helical coiled-coil heptad repeat on the interaction with membranes, and 3) the dynamics of coiled-coil peptide-membrane interactions depending on environmental conditions. Starting from an ideal alpha-helical coiled-coil peptide sequence, several positively charged analogues were designed that exhibit a high propensity toward negatively charged lipid membranes. Furthermore, these peptides differ in their ability to form a stable alpha-helical coiled-coil structure. The influence of a membrane environment on peptide folding is studied. All positively charged peptides show strong interactions with negatively charged membranes. This interaction induces an alpha-helical structure of the former random-coil peptides, as revealed by circular dichroism measurements. Furthermore, vesicle aggregation is induced by a coiled-coil interaction of vesicle-bound peptides. Dynamic light scattering experiments show that the strength of vesicle aggregation increases with the peptide's intrinsic ability to form a stable alpha-helical coiled coil. Thus, the peptide variant equipped with the strongest inter- and intra-helical coiled-coil interactions shows the strongest effect on vesicle aggregation. The secondary structure of this peptide in the membrane-bound state was studied as well as its effect on the phospholipids. Peptide conformation within the peptide-lipid aggregates was analyzed by (13)C cross-polarization magic-angle spinning NMR experiments. A uniformly (13)C- and (15)N-labeled Leu residue was introduced at position 12 of the peptide chain. The (13)C chemical shift and torsion angle measurements support the finding of an alpha-helical structure of the peptide in its membrane-bound state. Neither membrane leakage nor fusion was observed upon peptide binding, which is unusual for amphiphatic peptide structures. Our results lay the foundation for a systematic study of the influence of the alpha-helical coiled-coil folding motif in membrane-active events on a molecular level.