Insight into polyproline II helical bundle stability in an antifreeze protein denatured state

The use of polyproline II (PPII) helices in protein design is currently hindered by limitations in our understanding of their conformational stability and folding. Recent studies of the snow flea antifreeze protein (sfAFP), a useful model system composed of six PPII helices, suggested that a low denatured state entropy contributes to folding thermodynamics. Here, circular dichroism spectroscopy revealed minor populations of PPII like conformers at low temperature. To get atomic level information on the conformational ensemble and entropy of the reduced, denatured state of sfAFP, we have analyzed its chemical shifts and {¹H}-¹⁵N relaxation parameters by NMR spectroscopy at four experimental conditions. No significant populations of stable secondary structure were detected. The stiffening of certain N-terminal residues at neutral versus acidic pH and shifted pK_a values leads us to suggest that favorable charge-charge interactions could bias the conformational ensemble to favor the formation the C1-C28 disulfide bond during nascent folding, although no evidence for preferred contacts between these positions was detected by paramagnetic relaxation enhancement under denaturing conditions. Despite a high content of flexible glycine residues, the mobility of the sfAFP denatured ensemble is similar for denatured α/β proteins both on fast ps/ns as well as slower μs/ms timescales. These results are in line with a conformational entropy in the denatured ensemble resembling that of typical proteins and suggest that new structures based on PPII helical bundles should be amenable to protein design.     

Biochemistry of fish antifreeze proteins

Four distinct macromolecular antifreezes have been isolated and characterized from different marine fish. These include the glycoprotein antifreezes (Mr 2.5-33 K), which are made up of a repeating tripeptide (Ala-Ala-Thr)n with a disaccharide attached to the threonyl residues, and three antifreeze protein (AFP) types. Type I is an alanine-rich, amphiphilic, alpha-helix (Mr 3-5 K); type II is a larger protein (Mr 14 K) with a high content of reverse turns and five disulfide bridges; and type III is intermediate in size (Mr 6-7 K) with no distinguishing features of secondary structure or amino acid composition. Despite their marked structural differences, all four antifreeze types appear to function in the same way by binding to the prism faces of ice crystals and inhibiting growth along the a-axes. It is suggested that type I AFP binds preferentially to the prism faces as a result of interactions between the helix macrodipole and the dipoles on the water molecules in the ice lattice. Binding is stabilized by hydrogen bonding, and the amphiphilic character of the helix results in the hydrophobic phase of the helix being exposed to the solvent. When the solution temperature is lowered further, ice crystal growth occurs primarily on the uncoated, unordered basal plane resulting in bipyramidal-shaped crystals. The structural features of type I AFP that could contribute to this mechanism of action are reviewed. Current challenges lie in solving the other antifreeze structures and interpreting them in light of what appears to be a common mechanism of action.     

A rare polyglycine type II‐like helix motif in naturally occurring proteins

Common structural elements in proteins such as α‐helices or β‐sheets are characterized by uniformly repeating, energetically favorable main chain conformations which additionally exhibit a completely saturated hydrogen‐bonding network of the main chain NH and CO groups. Although polyproline or polyglycine type II helices (PP_II or PG_II) are frequently found in proteins, they are not considered as equivalent secondary structure elements because they do not form a similar self‐contained hydrogen‐bonding network of the main chain atoms. In this context our finding of an unusual motif of glycine‐rich PG_II‐like helices in the structure of the acetophenone carboxylase core complex is of relevance. These PG_II‐like helices form hexagonal bundles which appear to fulfill the criterion of a (largely) saturated hydrogen‐bonding network of the main‐chain groups and therefore may be regarded in this sense as a new secondary structure element. It consists of a central PG_II‐like helix surrounded by six nearly parallel PG_II‐like helices in a hexagonal array, plus an additional PG_II‐like helix extending the array outwards. Very related structural elements have previously been found in synthetic polyglycine fibers. In both cases, all main chain NH and CO groups of the central PG_II‐helix are saturated by either intra‐ or intermolecular hydrogen‐bonds, resulting in a self‐contained hydrogen‐bonding network. Similar, but incomplete PG_II‐helix patterns were also previously identified in a GTP‐binding protein and an antifreeze protein.     

Analysis and design of turns in alpha-helical hairpins

Although the analysis and design of turns that connect the strands in antiparallel beta-hairpins has reached an advanced state, much less is known concerning turns between antiparallel helices in helical hairpins. We have conducted an analysis of the structures and sequence preferences of two types of interhelical turns, each of which connects the two helices by a two-residue linker in an alphaL-beta conformation. Based on this analysis, it became apparent that the turn introduced into a designed four-helix bundle protein, DF1, did not occur within an optimal structural context. DF1 is a dimeric model for the diiron class of proteins. A longer loop with a beta-alphaR-beta conformation was inserted between two helices in the protein, and a sequence was chosen to stabilize its conformation. X-ray crystallography and NMR analysis of the protein showed the structure to be in excellent agreement with design.     

Crystal structure of thioredoxin from Escherichia coli at 1.68 A resolution

The crystal structure of thioredoxin from Escherichia coli has been refined by the stereochemically restrained least-squares procedure to a crystallographic R-factor of 0.165 at 1.68 A resolution. In the final model, the root-mean-square deviation from ideality for bond distances is 0.015 A and for angle distances 0.035 A. The structure contains 1644 protein atoms from two independent molecules, two Cu2+, 140 water molecules and seven methylpentanediol molecules. Ten residues have been modeled in two alternative conformations. E. coli thioredoxin is a compact molecule with 90% of its residues in helices, beta-strands or reverse turns. The molecule consists of two conformational domains, beta alpha beta alpha beta and beta beta alpha, connected by a single-turn alpha-helix and a 3(10) helix. The beta-sheet forms the core of the molecule packed on either side by clusters of hydrophobic residues. Helices form the external surface. The active site disulfide bridge between Cys32 and Cys35 is located at the amino terminus of the second alpha-helix. The positive electrostatic field due to the helical dipole is probably important for stabilizing the anionic intermediate during the disulfide reductase function of the protein. The more reactive cysteine, Cys32, has its sulfur atom exposed to solvent and also involved in a hydrogen bond with a backbone amide group. Residues 29 to 37, which include the active site cysteine residues, form a protrusion on the surface of the protein and make relatively fewer interactions with the rest of the structure. The disulfide bridge exhibits a right-handed conformation with a torsion angle of 81 degrees and 72 degrees about the S-S bond in the two molecules. Twenty-five pairs of water molecules obey the noncrystallographic symmetry. Most of them are involved in establishing intramolecular hydrogen-bonding interactions between protein atoms and thus serve as integral parts of the folded protein structure. Methylpentanediol molecules often pack against the loops and stabilize their structure. Cu2+ used for crystallization exhibit a distorted octahedral square bipyramid co-ordination and provide essential packing interactions in the crystal. The two independent protein molecules are very similar in conformation but distinctly different in atomic detail (root-mean-square = 0.94 A). The differences, which may be related to the crystal contacts, are localized mostly to regions far from the active site.     

The refined crystal structure of alpha-cobratoxin from Naja naja siamensis at 2.4-A resolution

The crystal structure of the "long" alpha-neurotoxin alpha-cobratoxin was refined to an R-factor of 19.5% using 3271 x-ray data to 2.4-A resolution. The polypeptide chain forms three loops, I, II, III, knotted together by four disulfide bridges, with the most prominent, loop II, containing another disulfide close to its lower tip. Loop I is stabilized by one beta-turn and two beta-sheet hydrogen bonds; loop II by eight beta-sheet hydrogen bonds, with the tip folded into two distorted right-handed helical turns stabilized by two alpha-helical and two beta-turn hydrogen bonds; and loop III by hydrophobic interactions and one beta-turn. Loop II and one strand of loop III form an antiparallel triple-pleated beta-sheet, and tight anchoring of the Asn63 side chain fixes the tail segment. In the crystal lattice, the alpha-cobratoxin molecules dimerize by beta-sheet formation between strands 53 and 57 of symmetry-related molecules. Because such interactions are found also in a cardiotoxin and alpha-bungarotoxin, this could be of importance for interaction with acetylcholine receptor.     

Chain-length dependence of alpha-helix to beta-sheet transition in polylysine: model of protein aggregation studied by temperature-tuned FTIR spectroscopy

The chain-length dependence of the alpha-helix to beta-sheet transition in poly(L-lysine) is studied by temperature-tuned FTIR spectroscopy. This study shows that heterogeneous samples of poly(L-lysine), comprising polypeptide chains with various lengths, undergo the alpha-beta transition at an intermediate temperature compared to homogeneous ingredients. This holds true as long as each individual fraction of the polypeptide is capable of adopting an antiparallel beta-sheet structure. The tendency is that the longer chain is, the lower the alpha-beta transition temperature is, which has been linked to the presence of distorted or solvated helices with turns or beta sheets in elongating chains of poly(L-lysine). As such helical structures are apparently conducive to the alpha-beta transition, this draws a comparison to the hypothesis of metastable protein conformational states being a common stage in amyloid-formation pathways. The antiparallel architecture of the beta sheet is likely to reflect the pretransition interhelical interactions in poly(L-lysine). Namely, the chains are arranged in an antiparallel manner because of energetically favored antiparallel pre-assembly of dipolar alpha helices.     

Disulfide bonds in a recombinant protein modeled after a core repeat in an aquatic insect's silk protein.

We constructed a gene encoding rCAS, recombinant constant and subrepeat protein, modeled after tandem repeats found in the major silk proteins synthesized by aquatic larvae of the midge, Chironomus tentans. Bacterially synthesized rCAS was purified to near homogeneity and characterized by several biochemical and biophysical methods including amino-terminal sequencing, amino acid compositional analysis, sedimentation equilibrium ultracentrifugation, and mass spectrometry. Complementing these techniques with quantitative sulfhydryl assays, we discovered that the four cysteines present in rCAS form two intramolecular disulfide bonds. Mapping studies revealed that the disulfide bonds are heterogeneous. When reduced and denatured rCAS was allowed to refold and its disulfide bonding state monitored, it again adopted a conformation with two intramolecular disulfide bonds. The inherent ability of rCAS to quantitatively form two intramolecular disulfide bonds may reflect a previously unknown feature of the in vivo silk proteins from which it is derived.     

Side-chain entropy effects on protein secondary structure formation

Loss of conformational entropy is one of the primary factors opposing protein folding. Both the backbone and side-chain of each residue in a protein will have their freedom of motion restricted in the final folded structure. The type of secondary structure of which a residue is part will have a significant impact on how much side-chain entropy is lost. Side-chain conformational entropies have previously been determined for folded proteins, simple models of unfolded proteins, alpha-helices, and a dipeptide model for beta-strands, but not for polyproline II (PII) helices. In this work, we present side-chain conformational estimates for the three regular secondary structure types: alpha-helices, beta-strands, and PII helices. Entropies are estimated from Monte Carlo computer simulations. Beta-strands are modeled as two structures, parallel and antiparallel beta-strands. Our data indicate that restraining a residue to the PII helix or antiparallel beta-strand conformations results in side-chain entropies equal to or higher than those obtained by restraining residues to the parallel beta-strand conformation. Side-chains in the alpha-helix conformation have the lowest side-chain entropies. The observation that extended structures retain the most side-chain entropy suggests that such structures would be entropically favored in unfolded proteins under folding conditions. Our data indicate that the PII helix conformation would be somewhat favored over beta-strand conformations, with antiparallel beta-strand favored over parallel. Notably, our data imply that, under some circumstances, residues may gain side-chain entropy upon folding. Implications of our findings for protein folding and unfolded states are discussed.     

YspD: A Potential Therapeutic Target for Drug Design to Combat Yersinia enterocolitica Infection

YspD is an annotated hydrophilic translocator of Ysa–Ysp type III secretion system of Yersinia enterocolitica. YspD has sequence, secondary structure and three-dimensional structure similar to other hydrophilic translocators. All hydrophilic translocators lack transmembrane region and possess intramolecular coiled-coil region. Disordered regions are mostly clustered at the N-terminal. Large loops provide flexibility, allowing conformational changes during oligomerization and protein–protein interaction. LcrV and PcrV have globular N-terminal and C-terminal domains, connected by intramolecular coiled-coil region. YspD, IpaD, SipD and BipD lack globular N-terminal and C-terminal domains. Their N-terminal and C-terminal domain have a bundle like structure connected by the intramolecular coiled-coil. The intramolecular coiled-coil regions (helix-5&9) of YspD showed maximum conservation, followed by helices at N-terminal. Polar interactions are mainly involved during dimerization of YspD, involving polar residues from helix-9 of both the YspD molecules. A methionine forms the boundary of interaction between the two YspD molecules. The two YspD molecules are arranged in antiparallel fashion to form the dimer. N-terminal of YspB interacted with C-terminal of YspD molecule to form a pentameric complex, consisting four YspD molecules and one YspB molecule. Sequence, structural similarity and presence of specific motifs in YspD (like chaperone protein) indicate the ability of N-terminal domain to show self-chaperoning activity and regulate folding and conformational state of YspD during its journey from the bacterial cytoplasm to the needle tip. Structural analysis of YspD and its mechanism of interaction with other proteins would enable us to design drugs against this hydrophilic protein to combat Yersinia infection.

     

Experimental and theoretical studies of the three-dimensional structure of human interleukin-4

The structure of human interleukin 4 (IL-4) was predicted utilizing a series of experimental and theoretical techniques. Circular Dichroism (CD) spectroscopy indicated that IL-4 belonged to the all alpha-helix class of protein structures. Secondary structure prediction, site-directed mutagenesis, and CD spectroscopy suggested a predominantly alpha-helical structure, consistent with a four-helix bundle structural motif. A human/mouse IL-4 chimera was constructed to qualitatively evaluate alternative secondary structure predictions. The four predicted helices were assembled into tertiary structures using established algorithms. The mapping of three disulfide bridges in IL-4 provided additional constraints on possible tertiary structures. Using accessible surface contact area as a criterion, the most suitable structures were right handed all antiparallel four-helix bundles with two overhand loop connections. Successful loop closure and incorporation of the three disulfide constraints were possible while maintaining the expected shape, solvent accessibility, and steric interactions between loops and helices. Lastly, energy minimization was used to regularize the chain.     

Discovery of a significant,nontopological preference for antiparallel alignment of helices with parallel regions in sheets

To help elucidate the role of secondary structure packing preferences in protein folding, here we present an analysis of the packing geometry observed between alpha-helices and between alpha-helices and beta-sheets in 1316 diverse, nonredundant protein structures. Finite-length vectors were fit to the alpha-carbon atoms in each of the helices and strands, and the packing angle between the vectors, Omega, was determined at the closest point of approach within each helix-helix or helix-sheet pair. Helix-sheet interactions were found in 391 of the proteins, and the distributions of Omega values were calculated for all the helix-sheet and helix-helix interactions. The packing angle preferences for helix-helix interactions are similar to those previously observed. However, analysis of helix-strand packing preferences uncovered a remarkable tendency for helices to align antiparallel to parallel regions of beta-sheets, independent of the topological constraints or prevalence of beta-alpha-beta motifs in the proteins. This packing angle preference is significantly diminished in helix interactions involving mixed and antiparallel beta-sheets, suggesting a role for helix-sheet dipole alignment in guiding supersecondary structure formation in protein folding. This knowledge of preferred packing angles can be used to guide the engineering of stable protein modules.     

Structure of variant-3 scorpion neurotoxin from Centruroides sculpturatus Ewing, refined at 1.8 A resolution

The three-dimensional structure of the variant-3 protein neurotoxin from the scorpion Centruroides sculpturatus Ewing has been determined by X-ray diffraction data. The initial model for the 65-residue protein was obtained at 3 A resolution by multiple-isomorphous-replacement methods. The structure was refined at 1.8 A resolution by restrained difference-Fourier methods, and by free-atom, block-diagonal least-squares. Considering the 4900 reflections for which d = 1.8-7 A and Fo greater than 2.5 sigma (Fo), the final R-index is 0.16 for the restrained model, and 0.14 for the free-atom model. Average estimated errors in atomic co-ordinates are about 0.1 A. The refined structure includes 492 protein atoms; one molecule of 2-methyl-2,4-pentanediol, which is tightly bound in a hydrophobic pocket on the surface of the protein; and 72 additional solvent sites. The major secondary structural features are two and a half turns of alpha-helix and a three-strand stretch of antiparallel beta-sheet. The helix is connected to the middle strand of the beta-sheet by two disulfide bridges, and a third disulfide bridge is located nearby. Several loops extend out of this dense core of secondary structure. The protein displays several reverse turns and a highly contorted proline-rich, COOH-terminal segment. One of the proline residues (Pro59) assumes a cis-conformation. The structure involves 44 intramolecular hydrogen bonds. The crystallographic results suggest two major corrections in the published primary structure; one of these has been confirmed by new chemical sequence data. The protein displays a large flattened surface that contains a high concentration of hydrophobic residues, along with most of the conserved amino acids that are found in the scorpion neurotoxins.     

Logical analysis of the mechanism of protein folding II. The nucleation process

Regions of secondary structure are predicted, without using information about the conformation of the protein itself, and compared with crystallographic assignments for seven proteins of recently published sequence and conformation (Table 1). It is observed in Table 3 that the prediction of helices is good (78.7% for %cor.ass.3), except for proteins having large antiparallel pleated sheets, and the prediction of β-structure is quite good (51.2% for %cor.ass.3) except for helix-rich proteins.The prediction of secondary structure from sequence, and a survey of all protein structures analysed so far by X-ray crystallography, suggest that nuceleation starts in almost all cases from interactions in the medium range between the regions having helical potential (α-candidate) and β-structural potential (β-candidate), which are very close to each other but separated by at least three hydrophilic or neutral residues in four consecutive residues on the polypeptide chain. Predictability of loops or turns is enhanced to 71.3% (%cor.ass.2) from 64.4% by taking into account the contiguous α-β interactions. Such a medium-range interaction is called here a probable nucleus. There are a lot of nuclei in large proteins such as carboxypeptidase Aα, while there exists at least one in small proteins like the trypsin inhibitor, Moreover, such an interaction could be a transitionary state towards a helix-rich protein, and towards a helix-deficient protein having a large antiparallel pleated sheet β-structure as well.The analysis of the relation between probable nuclei with regard to their mutual spatial proximity strongly suggests that the topological pathway of the polypeptide chain in three-dimensional space might be decided by the long-range interactions between an α-candidate and a β-candidate. An empirical rule is observed that almost all parallel pleated sheets are accompanied by helices in their neighbourhood. An accumulation of chemical facts, such as complementation experiments, combinations of disulphide bonds, etc., seems also to be elucidated by the proposed mechanism of protein folding.     

A simple model for polyproline II structure in unfolded states of alanine-based peptides

The striking similarity between observed circular dichroism spectra of nonprolyl homopolymers and that of regular left-handed polyproline II (P_II) helices prompted Tiffany and Krimm to propose in 1968 that unordered peptides and unfolded proteins are built of P_II segments linked by sharp bends. A large body of experimental evidence, accumulated over the past three decades, provides compelling evidence in support of the original hypothesis of Tiffany and Krimm. Of particular interest are the recent experiments of Shi et al. who find significant P_II structure in a short unfolded alanine-based peptide. What is the physical basis for P_II helices in peptide and protein unfolded states? The widely accepted view is that favorable chain-solvent hydrogen bonds lead to a preference for dynamical fluctuations about noncooperative P_II helices in water. Is this preference simply a consequence of hydrogen bonding or is it a manifestation of a more general trend for unfolded states which are appropriately viewed as chains in a good solvent? The prevalence of closely packed interiors in folded proteins suggests that under conditions that favor folding, water—which is a better solvent for itself than for any polypeptide chain—expels the chain from its midst, thereby maximizing chain packing. Implicit in this view is a complementary idea: under conditions that favor unfolding, chain-solvent interactions are preferred and in a so-called good solvent, chain packing density is minimized. In this work we show that minimization of chain packing density leads to preferred fluctuations for short polyalanyl chains around canonical, noncooperative P_II-like conformations. Minimization of chain packing is modeled using a purely repulsive soft-core potential between polypeptide atoms. Details of chain-solvent interactions are ignored. Remarkably, the simple model captures the essential physics behind the preference of short unfolded alanine-based peptides for P_II helices. Our results are based on a detailed analysis of the potential energy landscape which determines the system''s structural and thermodynamic preferences. We use the inherent structure formalism of Stillinger and Weber, according to which the energy landscape is partitioned into basins of attraction around local minima. We find that the landscape for the experimentally studied seven-residue alanine-based peptide is dominated by fluctuations about two noncooperative structures: the left-handed polyproline II helix and its symmetry mate.     

The extended left-handed helix: a simple nucleic acid-binding motif

The poly-proline type II extended left-handed helical structure is well represented in proteins. In an effort to determine the helix's role in nucleic acid recognition and binding, a survey of 258 nucleic acid-binding protein structures from the Protein Data Bank was conducted. Results indicate that left-handed helices are commonly found at the nucleic acid interfacial regions. Three examples are used to illustrate the utility of this structural element as a recognition motif. The third K homology domain of NOVA-2, the Epstein-Barr nuclear antigen-1, and the Drosophila paired protein homeodomain all contain left-handed helices involved in nucleic acid interactions. In each structure, these helices were previously unidentified as left-handed helices by secondary structure algorithms but, rather, were identified as either having small amounts of hydrogen bond patterns to the rest of the protein or as being "unstructured." Proposed mechanisms for nucleic acid interactions by the extended left-handed helix include both nonspecific and specific recognition. The observed interactions indicate that this secondary structure utilizes an increase in protein backbone exposure for nucleic acid recognition. Both main-chain and side-chain atoms are involved in specific and nonspecific hydrogen bonding to nucleobases or sugar-phosphates, respectively. Our results emphasize the need to classify the left-handed helix as a viable nucleic acid recognition and binding motif, similar to previously identified motifs such as the helix-turn-helix, zinc fingers, leucine zippers, and others.     

The relationship of the biophysical and biochemical characteristics of type VII collagen to the function of anchoring fibrils

Type VII collagen is a major component of anchoring fibrils, which are 800-nm-long centrosymmetrically cross-banded fibrils that are believed to secure the attachment of certain epithelial basement membranes to the underlying stromal matrix. The ultrastructure of the anchoring fibrils is highly variable, suggesting that the fibrils are flexible. Flexibility measurements along the length of the triple-helical domain of type VII procollagen indicate that major flexible sites correlate well with known discontinuities in the (Gly-X-Y)n repeating sequence. Therefore, the helical disruptions may account for the tortuous shapes of anchoring fibrils observed ultrastructurally. The centrosymmetrical banding pattern observed for anchoring fibrils results from the unstaggered lateral packing of antiparallel type VII collagen dimers that form these structures. This antiparallel arrangement is specified by disulfide bonds formed at the margins of a 60-nm overlap of the amino termini. As long as these disulfide bonds remain intact, they protect the amino-terminal overlapping triple helices from collagenase digestion. This disulfide-bonded pair of triple helices is termed C-1. Large nonhelical domains (NC-1) extend from both ends of the anchoring fibrils and are believed to interact with the basement membrane or with anchoring plaques. Rotary shadowing of the NC-1 domains showed trident-like shapes, suggesting that a single alpha-chain contributed the structure of each arm and that the three arms were extended. Biochemical and biophysical analyses of NC-1 domains independently confirm these suggestions and imply that the arms of NC-1 domains are identical and individually capable of interactions with basement membrane components, potentially allowing trivalent interaction of type VII collagen with various macromolecules.     

支持向量机方法预测蛋白质结构中的二硫键

在蛋白质结构预测的研究中,一个重要的问题就是正确预测二硫键的连接,二硫键的准确预测可以减少蛋白质构像的搜索空间,有利于蛋白质3D结构的预测,本文将预测二硫键的连接问题转化成对连接模式的分类问题,并成功地将支持向量机方法引入到预测工作中。通过对半胱氨酸局域序列连接模式的分类预测,可以由蛋白质的一级结构序列预测该蛋白质的二硫键的连接。结果表明蛋白质的二硫键的连接与半胱氨酸局域序列连接模式有重要联系,应用支持向量机方法对蛋白质结构的二硫键预测取得了良好的结果。     

Crystal structure of Z-Aib-Aib-Aib-Ala-Ala-Aib-OtBu, a hexapeptide fragment of trichotoxin

The crystal structure of Z-Aib-Aib-Aib-Ala-Ala-Aib-OtBu, an end-protected hexapeptide with a sequence corresponding to residues 7-12 of several trichotoxin A-50 sequence analogues has been determined by X-ray crystallography. The hexapeptide adopts a right-handed 3(10)-helical conformation consisting of four consecutive beta-turns of type III. The helix is stabilized by four intramolecular hydrogen bonds. In the crystal the molecules are connected head to tail with intermolecular hydrogen bonding interactions among translationally related molecules thus forming infinitely long helical columns. The column-column interactions in the crystal are hydrophobic and occur predominantly between antiparallel directed columns.     

Solution structure of cryptdin-4, a mouse paneth cell alpha-defensin

Mammalian defensins are abundant antimicrobial peptides that contribute to host defense. They are characterized by several conserved amino acids, including six invariant cysteine residues which form three intramolecular disulfide bonds and stabilize the tertiary structure. Cryptdin-4 (Crp4), a mouse alpha-defensin with potent in vitro bactericidal activity, has a primary structure distinct from all known alpha-defensins in that its polypeptide backbone uniquely lacks three residues between Cys(IV) and Cys(V). NMR diffusion experiments showed that Crp4 is monomeric in solution, and its three-dimensional solution structure, determined by two-dimensional proton NMR, consists of a triple-stranded antiparallel beta-sheet with the beta-strands joined to each other by a series of tight turns and a beta-hairpin. However, the overall beta-sheet content in Crp4 is lower than that of other alpha-defensin structures, while the shape and orientation of the Crp4 beta-hairpin also differ from those of other alpha-defensin structures. These structural characteristics combined with the high overall cationicity of Crp4 may contribute to its broad bactericidal spectrum and membrane disruptive activity.