Influence of strand number on antiparallel beta-sheet stability in designed three- and four-stranded beta-sheets

We describe experiments that probe whether antiparallel beta-sheet secondary structure becomes more stable as the number of strands increases. Several groups, including ours, have explored this issue with peptides designed to adopt three-stranded beta-sheet conformations, but the conclusions have not been consistent. In this study, we examine the effect on conformational stability of beta-sheet lengthening perpendicular to the strand direction via analysis of designed peptides that adopt three-stranded or four-stranded antiparallel beta-sheet conformations in aqueous solution. The findings reported here, along with the context provided by earlier studies, suggest that antiparallel beta-sheet does, in general, become more stable when the number of strands is increased from two to three. We show that this conclusion is not influenced by the rigidity of the loop segment used to link adjacent beta-strands (D-Pro-Gly versus Asn-Gly). We show that further extension, from three strands to four, leads to a further increase in antiparallel beta-sheet stability.     

The structure of bacterial outer membrane proteins

Integral membrane proteins come in two types, α-helical and β-barrel proteins. In both types, all hydrogen bonding donors and acceptors of the polypeptide backbone are completely compensated and buried while nonpolar side chains point to the membrane. The α-helical type is more abundant and occurs in cytoplasmic (or inner) membranes, whereas the β-barrels are known from outer membranes of bacteria. The β-barrel construction is described by the number of strands and the shear number, which is a measure for the inclination angle of the β-strands against the barrel axis. The common right-handed β-twist requires shear numbers slightly larger than the number of strands. Membrane protein β-barrels contain between 8 and 22 β-strands and have a simple topology that is probably enforced by the folding process. The smallest barrels form inverse micelles and work as enzymes or they bind to other macromolecules. The medium-range barrels form more or less specific pores for nutrient uptake, whereas the largest barrels occur in active Fe²⁺ transporters. The β-barrels are suitable objects for channel engineering, because the structures are simple and because many of these proteins can be produced into inclusion bodies and recovered therefrom in the exact native conformation.     

DEAD-box-protein-assisted RNA structure conversion towards and against thermodynamic equilibrium values

RNAs in biological processes often interconvert between defined structures. These RNA structure conversions are assisted by proteins and are frequently coupled to ATP hydrolysis. It is not well understood how proteins coordinate RNA structure conversions and which role ATP hydrolysis has in these processes. Here, we have investigated in vitro how the DEAD-box ATPase Ded1 facilitates RNA structure conversions in a simple model system. We find that Ded1 assists RNA structure conversions via two distinct pathways. One pathway requires ATP hydrolysis and involves the complete disassembly of the RNA strands. This pathway represents a kinetically controlled steady state between the RNA structures, which allows formation of less stable from more stable RNA conformations and thus RNA structure conversion against thermodynamic equilibrium values. The other pathway is ATP-independent and proceeds via multipartite intermediates that are stabilized by Ded1. Our results provide a basic mechanistic framework for protein-assisted RNA structure conversions that illuminates the role of ATP hydrolysis and reveal an unexpected diversity of pathways.     

The geometry of alpha-sheet: Implications for its possible function as amyloid precursor in proteins

alpha-sheet has been proposed as the main constituent of the prefibrillar intermediate during amyloid formation. Here the helical parameters of the alpha-sheet strand are calculated from average main-chain dihedral angles reported from molecular dynamics simulations. It is an almost linear polypeptide that forms a right-handed helix of about 100 A diameter, with 100 residues and a rise of 30 A per turn. The strands are curved but untwisted, which implies that neighboring strands need not coil to make interstrand hydrogen bonds. This suggests that compared to beta-sheets in native folded proteins, alpha-sheets can be larger and stack more easily to create extensive 3D blocks. It is shown that alpha-sheet is related to a category of structures termed "mirror" structures. Mirror structures have repetitive pairs of main-chain dihedral angles at residues i and i+1 that satisfy the condition phi(i) (+1) = -psi(i), psi(i) (+1) = -phi(i). They are uniquely identified by the two orientations of their peptide planes, specified by phi(i) and psi(i). Their side chains point alternately in opposite directions. Interestingly, their conformations are insensitive to phi(i) and psi(i) in that the pseudo dihedral angle formed by four consecutive C(alpha) atoms is always close to 180 degrees . There are two types: "beta-mirror" and "alpha-mirror" structure; beta-mirror structures relate to beta-sheet by small peptide plane rotations, of less than 90 degrees , while alpha-mirror structures are close to alpha-sheet and relate to beta-sheet by approximately 180 degrees peptide plane flips. Most mirror structures, and in particular the alpha-mirror, form wide helices with diameters 50-70 A. Their gentle curvature, and therefore that of the alpha-sheet, arises from the orientation of successive peptide units causing the difference in the bond angles at the C and N atoms of the peptide unit to gradually change the direction of the chain.     

Side-chain control of beta-peptide secondary structures.

As one of the most important families of non-natural polymers with the propensity to form well-defined secondary structures, the beta-peptides are attracting increasing attention. The compounds incorporating beta-amino acid residues have found various applications in medicinal chemistry and biochemistry. The conformational pool of beta-peptides comprises several periodic folded conformations, which can be classified as helices, and nonpolar and polar strands. The latter two are prone to form pleated sheets. The numerous studies that have been performed on the side-chain dependence of the stability of the folded structures allow certain conclusions concerning the principles of design of the beta-peptide foldamers. The folding propensity is influenced by local torsional, side-chain to backbone and long-range side-chain interactions. Although beta-peptide foldamers are sensitive to solvent, the systematic choice of the side-chain pattern and spatiality allows the design of the desired specific secondary structure. The application of beta-peptide foldamers may open up new directions in the synthesis of highly organized artificial tertiary structures with biochemical functions.     

''A'' forms of RNAs in single strands, duplexes and RNA-DNA hybrids.

Helical parameters have been calculated for the 'A' form minimum energy conformations of ApA, CpC, GpG, UpU, GpC and UpA. The helix geometries are base sequence dependent. The single strands are narrower and more tightly wound than that duplex RNA-11 form. 9-12 kcal./mole are needed to convert these single strands to the RNA-11 conformation. However, in some sequences other 'A' type conformers capable of complementary base pairing may be formed at lower energetic cost. There is substantially more base stacking in the calculated single strands than in the RNA-11 conformation. Calculated intrastrand base stacking energies reflect these differences, and also are sequence dependent. The 'A' form RNA subunits differ from the analogous DNAs in possessing a larger rise per residue, needed to accomodate the 2'-OH. RNA-DNA hybrids are consequently more likely to be in the 'A-RNA than in the 'A'-DNA conformation, although the base sequence determines the extent of the preference.     

Comparison of two highly refined structures of bovine pancreatic trypsin inhibitor

The high resolution structures of bovine pancreatic trypsin inhibitor refined in two distinct crystal forms have been compared. One of the structures was a result of new least-squares X-ray refinement of data from crystal form I, while the other was the joint X-ray/neutron structure of crystal form II. After superposition, the molecules show an overall root-mean-squares deviation of 0.40 A for the atoms in the main chain, while the deviations for the side-chain atoms are 1.53 A. The latter number decreases to 0.61 A when those side-chains that adopted drastically different conformations are excluded from comparison. The discrepancy between atomic temperature factors in the two models was 6.7 A2, while their general trends are highly correlated. About half of the solvent molecules occupy similar positions in the two models, while the others are different. As expected, solvents with the lowest temperature factors are most likely to be common in the two crystal forms. While the two models are clearly similar, the differences are significantly larger than the errors inherent in the structure determination.     

Antifreeze protein from freeze-tolerant grass has a beta-roll fold with an irregularly structured ice-binding site

The grass Lolium perenne produces an ice-binding protein (LpIBP) that helps this perennial tolerate freezing by inhibiting the recrystallization of ice. Ice-binding proteins (IBPs) are also produced by freeze-avoiding organisms to halt the growth of ice and are better known as antifreeze proteins (AFPs). To examine the structural basis for the different roles of these two IBP types, we have solved the first crystal structure of a plant IBP. The 118-residue LpIBP folds as a novel left-handed beta-roll with eight 14- or 15-residue coils and is stabilized by a small hydrophobic core and two internal Asn ladders. The ice-binding site (IBS) is formed by a flat beta-sheet on one surface of the beta-roll. We show that LpIBP binds to both the basal and primary-prism planes of ice, which is the hallmark of hyperactive AFPs. However, the antifreeze activity of LpIBP is less than 10% of that measured for those hyperactive AFPs with convergently evolved beta-solenoid structures. Whereas these hyperactive AFPs have two rows of aligned Thr residues on their IBS, the equivalent arrays in LpIBP are populated by a mixture of Thr, Ser and Val with several side-chain conformations. Substitution of Ser or Val for Thr on the IBS of a hyperactive AFP reduced its antifreeze activity. LpIBP may have evolved an IBS that has low antifreeze activity to avoid damage from rapid ice growth that occurs when temperatures exceed the capacity of AFPs to block ice growth while retaining the ability to inhibit ice recrystallization.     

Solvent accessibility in native and isolated domain environments: general features and implications to interface predictability

A non-redundant database of 4536 structural domains, comprising more than 790,000 residues, has been used for the calculation of their solvent accessibility in the native protein environment and then in the isolated domain environment. Nearly 140,000 (18%) residues showed a change in accessible surface area in the above two conditions. General features of this change under these two circumstances have been pointed out. Propensities of these interfacing amino acid residues have been calculated and their variation for different secondary structure types has been analyzed. Actual amount of surface area lost by different secondary structures is higher in the case of helix and strands compared to coil and other conformations. Overall change in surface area in hydrophobic and uncharged residues is higher than that in charged residues. An attempt has been made to know the predictability of interface residues from sequence environments. This analysis and prediction results have significant implications towards determining interacting residues in proteins and for the prediction of protein-protein, protein-ligand, protein-DNA and similar interactions.     

Molecular dynamics simulation of the SH3 domain aggregation suggests a generic amyloidogenesis mechanism

We use molecular dynamics simulation to study the aggregation of Src SH3 domain proteins. For the case of two proteins, we observe two possible aggregation conformations: the closed form dimer and the open aggregation state. The closed dimer is formed by "domain swapping"-the two proteins exchange their RT-loops. All the hydrophobic residues are buried inside the dimer so proteins cannot further aggregate into elongated amyloid fibrils. We find that the open structure-stabilized by backbone hydrogen bond interactions-packs the RT-loops together by swapping the two strands of the RT-loop. The packed RT-loops form a beta-sheet structure and expose the backbone to promote further aggregation. We also simulate more than two proteins, and find that the aggregate adopts a fibrillar double beta-sheet structure, which is formed by packing the RT-loops from different proteins. Our simulations are consistent with a possible generic amyloidogenesis scenario.     

NMR structure of the full-length linear dimer of stem-loop-1 RNA in the HIV-1 dimer initiation site

The packaging signal of HIV-1 RNA contains a stem-loop structure, SL1, which serves as the dimerization initiation site for two identical copies of the genome and is important for packaging of the RNA genome into the budding virion and for overall infectivity. SL1 spontaneously dimerizes via a palindromic hexanucleotide sequence in its apical loop, forming a metastable kissing dimer form. Incubation with nucleocapsid protein causes this form to refold to a thermodynamically stable mature linear dimer. Here, we present an NMR structure of the latter form of the full-length SL1 sequence of the Lai HIV-1 isolate. The structure was refined using nuclear Overhauser effect and residual dipolar coupling data. The structure presents a symmetric homodimer of two RNA strands of 35 nucleotides each; it includes five stems separated by four internal loops. The central palindromic stem is surrounded by two symmetric adenine-rich 1-2 internal loops, A-bulges. All three adenines in each A-bulge are stacked inside the helix, consistent with the solution structures of shorter SL1 constructs determined previously. The outer 4-base pair stems and, proximal to them, purine-rich 1-3 internal loops, or G-bulges, are the least stable parts of the molecule. The G-bulges display high conformational variability in the refined ensemble of structures, despite the availability of many structural restraints for this region. Nevertheless, most conformations share a similar structural motif: a guanine and an adenine from opposite strands form a GA mismatch stacked on the top of the neighboring stem. The two remaining guanines are exposed, one in the minor groove and another in the major groove side of the helix, consistent with secondary structure probing data for SL1. These guanines may be recognized by the nucleocapsid protein, which binds tightly to the G-bulge in vitro.     

Conformational polymorphism in telomeric structures: Loop orientation and interloop pairing in d(G4TnG4)

Sequence repeats constituting the telomeric regions of chromosomes are known to adopt a variety of unusual structures, consisting of a G tetraplex stem and short stretches of thymines or thymines and adenines forming loops over the stem. Detailed model building and molecular mechanics studies have been carried out for these telomeric sequences to elucidate different types of loop orientations and possible conformations of thymines in the loop. The model building studies indicate that a minimum of two thymines have to be interspersed between guanine stretches to form folded-back structures with loops across adjacent strands in a G tetraplex (both over the small as well as large groove), while the minimum number of thymines required to build a loop across the diagonal strands in a G tetraplex is three. For two repeat sequences, these hairpins, resulting from different types of folding, can dimerize in three distinct ways—i.e., with loops across adjacent strands and on same side, with loops across adjacent strands and on opposite sides, and with loops across diagonal strands and on opposite sides—to form hairpin dimer structures. Energy minimization studies indicate that all possible hairpin dimers have very similar total energy values, though different structures are stabilized by different types of interactions. When the two loops are on the same side, in the hairpin dimer structures of d(G₄T_nG₄), the thymines form favorably stacked tetrads in the loop region and there is interloop hydrogen bonding involving two hydrogen bonds for each thymine–thymine pair. Our molecular mechanics calculations on various folded-back as well as parallel tetraplex structures of these telomeric sequences provide a theoretical rationale for the experimentally observed feature that the presence of intervening thymine stretches stabilizes folded-back structures, while isolated stretches of guanines adopt a parallel tetraplex structure. © 1994 John Wiley & Sons, Inc.     

Role of medium--and long-range interactions in discriminating globular and membrane proteins.

The analysis of inter-residue interactions in protein structures provides considerable insight to understand their folding and stability. We have previously analyzed the role of medium- and long-range interactions in the folding of globular proteins. In this work, we study the distinct role of such interactions in the three-dimensional structures of membrane proteins. We observed a higher number of long-range contacts in the termini of transmembrane helical (TMH) segments, implying their role in the stabilization of helix-helix interactions. The transmembrane strand (TMS) proteins are having appreciably higher long-range contacts than that in all-beta class of globular proteins, indicating closer packing of the strands in TMS proteins. The residues in membrane spanning segments of TMH proteins have 1.3 times higher medium-range contacts than long-range contacts whereas that of TMS proteins have 14 times higher long-range contacts than medium-range contacts. Residue-wise analysis indicates that in TMH proteins, the residues Cys, Glu, Gly, Pro, Gln, Ser and Tyr have higher long-range contacts than medium-range contacts in contrast with all-alpha class of globular proteins. The charged residue pairs have higher medium-range contacts in all-alpha proteins, whereas hydrophobic residue pairs are dominant in TMH proteins. The information on the preference of residue pairs to form medium-range contacts has been successfully used to discriminate the TMH proteins from all-alpha proteins. The statistical significance of the results obtained from the present study has been verified using randomized structures of TMH and TMS protein templates.     

The turn of the screw: variations of the abundant beta-solenoid motif in passenger domains of Type V secretory proteins

Many virulence factors of gram-negative bacteria are secreted by the Type V secretion system via the autotransporter (AT) and two-partner secretion (TPS) pathways. AT proteins effect their own secretion. They comprise three domains: the amino-terminal leader sequence; the secreted passenger domain; and the translocator domain that forms the secretory channel. In the TPS pathway, the passenger and translocator domains are translated as separate proteins. In a previous publication, we proposed a beta-helical structure for the TPS passenger domain of the filamentous hemagglutinin (FHA) of Bordetella pertussis which contains two tracts, R1 and R2, of 19-residue sequence repeats and built molecular models for the R1 and R2 beta-helices. Here, we compare the structure predicted for R1 with the recently determined crystal structure of a fragment containing three R1 repeats and find close agreement, with an RMSD of 1.1A. In the interim, the number of known AT and TPS protein sequences has increased to >1000. To investigate the incidence of beta-helical structures among them, we carried out a sequence-based analysis and conclude that, despite wide diversity in the sizes and sequences of passenger domains, most of them contain beta-solenoids that we classify into thirteen types based on distinctive properties of their beta-coils (repeat length, numbers and lengths of beta-strands and turns, cross-sectional shape, presence of specific residues in certain positions) summarized in a 2D coil template. Some coil types are typical for conventional AT proteins, others, for TPS or trimeric AT proteins. Some beta-solenoids consist of stacked subdomains with coils of different types. To illustrate model-building from a coil template, we modeled a type-T4 beta-solenoid for TibA of Escherichia coli which is predicted to have two conserved polar residues, Thr and Gln, in interior positions.     

Assembly and characterization of five-arm and six-arm DNA branched junctions.

DNA branched junctions have been constructed that contain either five arms or six arms surrounding a branch point. These junctions are not as stable as junctions containing three or four arms; unlike the smaller junctions, they cannot be shown to migrate as a single band on native gels when each of their arms contains eight nucleotide pairs. However, they can be stabilized if their arms contain 16 nucleotide pairs. Ferguson analysis of these junctions in combination with three-arm and four-arm junctions indicates a linear increase in friction constant as the number of arms increases, with the four-arm junction migrating anomalously. The five-arm junction does not appear to have any unusual stacking structure, and all strands show similar responses to hydroxyl radical autofootprinting analysis. By contrast, one strand of the six-arm junction shows virtually no protection from hydroxyl radicals, suggesting that it is the helical strand of a preferred stacking domain. Both junctions are susceptible to digestion by T4 endonuclease VII, which resolves Holliday junctions. However, the putative helical strand of the six-arm junction shows markedly reduced cleavage, supporting the notion that its structure is largely found in a helical conformation. Branched DNA molecules can be assembled into structures whose helix axes form multiply connected objects and networks. The ability to construct five-arm and six-arm junctions vastly increases the number of structures and networks that can be built from branched DNA components. Icosahedral deltahedra and 11 networks with 432 symmetry, constructed from Platonic and Archimedean solids, are among the structures whose construction is feasible, now that these junctions can be made.     

Three-dimensional structure of α-crystallin domain dimers of human small heat shock proteins HSPB1 and HSPB6

Small heat shock proteins (sHSPs) are a family of evolutionary conserved ATP-independent chaperones. These proteins share a common architecture defined by a signature α-crystallin domain (ACD) flanked by highly variable N- and C-terminal extensions. The ACD, which has an immunoglobulin-like fold, plays an important role in sHSP assembly. This domain mediates dimer formation of individual protomers, which then may assemble into larger oligomers. In vertebrate sHSPs, the dimer interface is formed by the symmetrical antiparallel pairing of two β-strands (β7), generating an extended β-sheet on one face of the ACD dimer. Recent structural studies of isolated ACDs from a number of vertebrate sHSPs suggest a variability in the register of the β7/β7 strand interface, which may, in part, give rise to the polydispersity often associated with the full-length proteins. To further analyze the structure of ACD dimers, we have employed a combination of X-ray crystallography and solution small-angle X-ray scattering (SAXS) to study the ACD-containing fragments of human HSPB1 (HSP27) and HSPB6 (HSP20). Unexpectedly, the obtained crystal structure of the HSPB1 fragment does not reveal the typical β7/β7 dimers but, rather, hexamers formed by an asymmetric contact between the β4 and the β7 strands from adjacent ACDs. Nevertheless, in solution, both ACDs form stable dimers via the symmetric antiparallel interaction of β7 strands. Using SAXS, we show that it is possible to discriminate between different putative registers of the β7/β7 interface, with the results indicating that, under physiological conditions, there is only a single register of the strands for both proteins.     

Structural compromise of disallowed conformations in peptide and protein structures

Using a data set of 454 crystal structures of peptides and 80 crystal structures of non-homologous proteins solved at ultra high resolution of 1.2 A or better we have analyzed the occurrence of disallowed Ramachandran (phi, psi) angles. Out of 1492 and 13508 non-glycyl residues in peptides and proteins respectively 12 and 76 residues in the two datasets adopt clearly disallowed combinations of Ramachandran angles. These examples include a number of conformational points which are far away from any of the allowed regions in the Ramachandran map. According to the Ramachandran map a given (phi, psi) combination is considered disallowed when two non-bonded atoms in a system of two-linked peptide units with ideal geometry are prohibitively proximal in space. However, analysis of the disallowed conformations in peptide and protein structures reveals that none of the observations of disallowed conformations in the crystal structures correspond to a short contact between non-bonded atoms. A further analysis of deviations of bond lengths and angles, from the ideal peptide geometry, at the residue positions of disallowed conformations in the crystal structures suggest that individual bond lengths and angles are all within acceptable limits. Thus, it appears that the rare tolerance of disallowed conformations is possible by gentle and acceptable deviations in a number of bond lengths and angles, from ideal geometry, over a series of bonds resulting in a net gross effect of acceptable non-bonded inter-atomic distances.     

Structural study of four-stranded quadruplex structures containing 2'-deoxy-8-(propyn-1-yl)adenosine

In this paper, we report the NMR structural study of two quadruplex structures formed by truncations of the human telomeric sequence and containing a modified base, namely d(AprGGGT) and d(TAprGGGT), where Apr indicates 2'-deoxy-8-(propyn-1-yl)adenosines. Both oligonucleotides have been found to form 4-fold symmetric G-quadruplex structures with all strands parallel and equivalent to each other and characterized by higher thermal stabilities than the natural counterparts. The presence of the propynyl groups affects the conformations of the 5' edge of both quadruplexes in such a way to prevent the formation of one of the two possible H-bond patterns observed for a canonical A-tetrad. The increased thermal stabilities of the modified quadruplexes seem to be mostly due to a prevalent syn glycosidic conformation assumed by the Apr residues.     

Structural diversity of sequentially identical subsequences of proteins: Identical octapeptides can have different conformations

One of the most important questions in the protein folding problem is whether secondary structures are formed entirely by local interactions. One way to answer this question is to compare identical subsequences of proteins to see if they have identical structures. Such an exercise would also reveal a lower limit on the number of amino acids needed to form unique secondary structures. In this context, we have searched the April 1996 release of the Protein Data Bank for sequentially identical subsequences of proteins and compared their structures. We find that identical octamers can have different conformations. In addition, there are several examples of identical heptamers with different conformations, and the number of identical hexamers with different conformations has increased since the previous PDB releases. These observations imply that secondary structure can be formed entirely by non-local interactions and that an identical match of up to eight amino acids may not imply structural similarity. In addition to the larger context of the protein folding problem, these observations have implications for protein structure prediction methods. Proteins 30:228–231, 1998. © 1998 Wiley-Liss, Inc.     

The Common Architecture of Cross-β Amyloid

Amyloid fibril deposition is central to the pathology of more than 30 unrelated diseases including Alzheimer's disease and Type 2 diabetes. It is generally accepted that amyloid fibrils share common structural features despite each disease being characterised by the deposition of an unrelated protein or peptide. The structure of amyloid fibrils has been studied using X-ray fibre diffraction and crystallography, solid-state NMR and electron paramagnetic resonance, and many different, sometimes opposing, models have been suggested. Many of these models are based on the original interpretation of the cross-β diffraction pattern for cross-β silk in which β-strands run perpendicular to the fibre axis, although alternative models include β-helices and natively structured proteins. Here, we have analysed opposing model structures and examined the necessary structural elements within the amyloid core structure, as well as producing idealised models to test the limits of the core conformation. Our work supports the view that amyloid fibrils share a number of common structural features, resulting in characteristic diffraction patterns. This pattern may be satisfied by structures in which the strands align close to perpendicular to the fibre axis and are regularly arranged to form β-sheet ribbons. Furthermore, the fibril structure contains several β-sheets that associate via side-chain packing to form the final protofilament structure.