Influence of Nonconserved Regions of L1 Protuberance of <Emphasis Type="Italic">Thermus thermophilus</Emphasis> Ribosome on the Affinity of L1 Protein to 23s rRNA

The L1 protuberance of the ribosome includes two domain ribosomal protein L1 and three helices of 23S rRNA (H76, H77, and H78) with interconnecting loops A and B. Helix 78 consists of two parts, i.e., H78a and H78b. A comparison of the available structural data of L1-RNA complexes with the obtained kinetic data made it possible to determine the influence of the nonconserved regions of Thermus thermophilus L1-protuberance on the mutual affinity of the L1 protein and 23S rRNA. It has been shown that the N-terminal helix of the protein and 78b helix of 23S rRNA are essential for the formation of an additional intermolecular contact, which is separated in the protein from the main site of L1-rRNA interaction by a flexible connection. This results in a rise in the TthL1-rRNA affinity. At the same time, the elongation of the 76 helix has no effect on rRNA-protein binding.     

Impact of bulge loop size on DNA triplet repeat domains: Implications for DNA repair and expansion

Repetitive DNA sequences exhibit complex structural and energy landscapes, populated by metastable, noncanonical states, that favor expansion and deletion events correlated with disease phenotypes. To probe the origins of such genotype–phenotype linkages, we report the impact of sequence and repeat number on properties of (CNG) repeat bulge loops. We find the stability of duplexes with a repeat bulge loop is controlled by two opposing effects; a loop junction‐dependent destabilization of the underlying double helix, and a self‐structure dependent stabilization of the repeat bulge loop. For small bulge loops, destabilization of the underlying double helix overwhelms any favorable contribution from loop self‐structure. As bulge loop size increases, the stabilizing loop structure contribution dominates. The role of sequence on repeat loop stability can be understood in terms of its impact on the opposing influences of junction formation and loop structure. The nature of the bulge loop affects the thermodynamics of these two contributions differently, resulting in unique differences in repeat size‐dependent minima in the overall enthalpy, entropy, and free energy changes. Our results define factors that control repeat bulge loop formation; knowledge required to understand how this helix imperfection is linked to DNA expansion, deletion, and disease phenotypes. © 2013 Wiley Periodicals, Inc. Biopolymers 101: 1–12, 2014.     

Conservation of helical structure contributes to functional metal ion interactions in the catalytic domain of ribonuclease P RNA

Like protein enzymes, catalytic RNAs contain conserved structure motifs important for function. A universal feature of the catalytic domain of ribonuclease P RNA is a bulged-helix motif within the P1-P4 helix junction. Here, we show that changes in bulged nucleotide identity and position within helix P4 affect both catalysis and substrate binding, while a subset of the mutations resulted only in catalytic defects. We find that the proximity of the bulge to sites of metal ion coordination in P4 is important for catalysis; moving the bulge distal to these sites and deleting it had similarly large effects, while moving it proximal to these sites had only a moderate effect on catalysis. To test whether the effects of the mutations are linked to metal ion interactions, we used terbium-dependent cleavage of the phosphate backbone to probe metal ion-binding sites in the wild-type and mutant ribozymes. We detect cleavages at specific sites within the catalytic domain, including helix P4 and J3/4, which have previously been shown to participate directly in metal ion interactions. Mutations introduced into P4 cause local changes in the terbium cleavage pattern due to alternate metal ion-binding configurations with the helix. In addition, a bulge deletion mutation results in a 100-fold decrease in the single turnover cleavage rate constant at saturating magnesium levels, and a reduced affinity for magnesium ions important for catalysis. In light of the alternate terbium cleavage pattern in P4 caused by bulge deletion, this decreased ability to utilize magnesium ions for catalysis appears to be due to localized structural changes in the ribozyme's catalytic core that weaken metal ion interactions in P4 and J3/4. The information reported here, therefore, provides evidence that the universal conservation of the P4 structure is based in part on optimization of metal ion interactions important for catalysis.     

Structural basis for the function of the ribosomal L7/12 stalk in factor binding and GTPase activation

The L7/12 stalk of the large subunit of bacterial ribosomes encompasses protein L10 and multiple copies of L7/12. We present crystal structures of Thermotoga maritima L10 in complex with three L7/12 N-terminal-domain dimers, refine the structure of an archaeal L10E N-terminal domain on the 50S subunit, and identify these elements in cryo-electron-microscopic reconstructions of Escherichia coli ribosomes. The mobile C-terminal helix alpha8 of L10 carries three L7/12 dimers in T. maritima and two in E. coli, in concordance with the different length of helix alpha8 of L10 in these organisms. The stalk is organized into three elements (stalk base, L10 helix alpha8-L7/12 N-terminal-domain complex, and L7/12 C-terminal domains) linked by flexible connections. Highly mobile L7/12 C-terminal domains promote recruitment of translation factors to the ribosome and stimulate GTP hydrolysis by the ribosome bound factors through stabilization of their active GTPase conformation.     

Solution structure of subunit F(6) from the peripheral stalk region of ATP synthase from bovine heart mitochondria

The ATP synthase enzyme structure includes two stalk assemblies, the central stalk and the peripheral stalk. Catalysis involves rotation of the central stalk assembly together with the membrane-embedded ring of c-subunits driven by the trans-membrane proton-motive force, while the alpha and beta-subunits of F(1) are prevented from co-rotating by their attachment to the peripheral stalk. In the absence of structures of either the intact peripheral stalk or larger complexes containing it, we are studying its individual components and their interactions to build up an overall picture of its structure. Here, we describe an NMR structural characterisation of F(6), which is a 76-residue protein located in the peripheral stalk of the bovine ATP synthase and is essential for coupling between the proton-motive force and catalysis. Isolated F(6) has a highly flexible structure comprising two helices packed together through a loose hydrophobic core and connected by an unstructured linker. Analysis of chemical shifts, (15)N relaxation and RDC measurements confirm that the F(6) structure is flexible on a wide range of timescales ranging from nanoseconds to seconds. The relationship between this structure for isolated F(6) and its role in the intact peripheral stalk is discussed.     

Trapping the on-pathway folding intermediate of Im7 at equilibrium

The four-helical protein Im7 folds via a rapidly formed on-pathway intermediate (k(UI)=3000 s(-1) at pH 7.0, 10 degrees C) that contains three (helices I, II and IV) of the four native alpha-helices. The relatively slow (k(IN)=300 s(-1)) conversion of this intermediate into the native structure is driven by the folding and docking of the six residue helix III onto the developing hydrophobic core. Here, we describe the structural properties of four Im7* variants designed to trap the protein in the intermediate state by disrupting the stabilising interactions formed between helix III and the rest of the protein structure. In two of these variants (I54A and L53AI54A), hydrophobic residues within helix III have been mutated to alanine, whilst in the other two mutants the sequence encompassing the native helix III was replaced by a glycine linker, three (H3G3) or six (H3G6) residues in length. All four variants were shown to be monomeric, as judged by analytical ultracentrifugation, and highly helical as measured by far-UV CD. In addition, all the variants denature co-operatively and have a stability (DeltaG(UF)) and buried hydrophobic surface area (M(UF)) similar to those of the on-pathway kinetic intermediate. Structural characterisation of these variants using 1-anilino-8-napthalene sulphonic acid (ANS) binding, near-UV CD and 1D (1)H NMR demonstrate further that the trapped intermediate ensemble is highly structured with little exposed hydrophobic surface area. Interestingly, however, the structural properties of the variants I54A and L53AI54A differ in detail from those of H3G3 and H3G6. In particular, the single tryptophan residue, located near the end of helix IV, and distant from helix III, is in a distinct environment in the two sets of mutants as judged by fluorescence, near-UV CD and the sensitivity of tryptophan fluorescence to iodide quenching. Overall, the results confirm previous kinetic analysis that demonstrated the hierarchical folding of Im7 via an on-pathway intermediate, and show that this species is a highly helical ensemble with a well-formed hydrophobic core. By contrast with the native state, however, the intermediate ensemble is flexible enough to change in response to mutation, its structural properties being tailored by residues in the sequence encompassing the native helix III.     

Deoxymyoglobin studied by the conformational normal mode analysis. I. Dynamics of globin and the heme-globin interaction

Dynamic properties of deoxymyoglobin are studied theoretically by the analysis of conformational fluctuations. Root-mean-square atomic fluctuations and distance fluctuations between different segments reveal the mechanical construction of the molecule. Eight alpha-helices behave as relatively rigid bodies and corner regions are more flexible, showing larger fluctuations. More particularly, corner regions EF and GH are specific in that flanking alpha-helices extend their rigidity up to a point in the corner region and the two rigid segments are connected flexibly at that point. The FG corner is exceptional. A segment from the F helix to the beginning of the G helix, in which the FG corner is included, becomes relatively rigid by means of strong interactions with the heme group. The whole myoglobin molecule is divided into two large units of motion, one extending from the B to the E helix, and the other from the F to the H helix. These two units are connected covalently by the EF corner. However, dynamic interactions between these two units take place mainly through contacts between helices B and G and not through the EF corner. From correlation coefficients between fluctuational motions of residues and the heme group, 55 residues are identified as having strong dynamic interactions with the heme moiety. Among them, 18 residues in the three segments, one consisting of residues from the C helix to the CD corner, a second consisting of the E helix, and a third from the F helix to the beginning of the G helix, are in close contact with the heme group. Twenty-two of the 55 residues are within four residues of the 18 residues in their sequential residue number and are more than 3 A away from the heme group. The other 15 residues are located further in the sequential residue number and are all found in helices A and H. They are more than 6 A away from the heme group. By the use of correlation coefficients of fluctuations between residues, it is found that dynamic interaction with the heme group is transmitted to the A helix and the beginning of the H helix in the direction Leu(E15)----[Val(All) and Trp(A12)]. The transmission to the C-terminal end of the H helix is mediated by a long segment, from the end of the EF corner to the beginning of the G helix, that lies on the heme group and has close contacts over a wide range.(ABSTRACT TRUNCATED AT 400 WORDS)     

X-ray structure of full-length annexin 1 and implications for membrane aggregation

Annexins comprise a multigene family of Ca2+ and phospholipid- binding proteins. They consist of a conserved C-terminal or core domain that confers Ca2+-dependent phospholipid binding and an N-terminal domain that is variable in sequence and length and responsible for the specific properties of each annexin. Crystal structures of various annexin core domains have revealed a high degree of similarity. From these and other studies it is evident that the core domain harbors the calcium-binding sites that interact with the phospholipid headgroups. However, no structure has been reported of an annexin with a complete N-terminal domain. We have now solved the crystal structure of such a full-length annexin, annexin 1. Annexin 1 is active in membrane aggregation and its refined 1.8 A structure shows an alpha-helical N-terminal domain connected to the core domain by a flexible linker. It is surprising that the two alpha-helices present in the N-terminal domain of 41 residues interact intimately with the core domain, with the amphipathic helix 2-12 of the N-terminal domain replacing helix D of repeat III of the core. In turn, helix D is unwound into a flap now partially covering the N-terminal helix. Implications for membrane aggregation will be discussed and a model of aggregation based on the structure will be presented.     

NMR analysis of the conformational properties of the trapped on-pathway folding intermediate of the bacterial immunity protein Im7

Previous work shows that the transiently populated, on-pathway intermediate in Im7 folding contains three of the four native alpha-helices docked around a core stabilised by native and non-native interactions. To determine the structure and dynamic properties of this species in more detail, we have used protein engineering to trap the intermediate at equilibrium and analysed the resulting proteins using NMR spectroscopy and small angle X-ray scattering. Four variants were created. In L53AI54A, two hydrophobic residues within helix III are truncated, preventing helix III from docking stably onto the developing hydrophobic core. In two other variants, the six residues encompassing the native helix III were replaced with three (H3G3) or six (H3G6) glycine residues. In the fourth variant, YY, two native tyrosine residues (Tyr55 and Tyr56) were re-introduced into H3G6 to examine their role in determining the properties of the intermediate ensemble. All four variants show variable peak intensities and broad peak widths, consistent with these proteins being conformationally dynamic. Chemical shift analyses demonstrated that L53AI54A and YY contain native-like secondary structure in helices I and IV, while helix II is partly formed and helix III is absent. Lack of NOEs and rapid NH exchange for L53AI54A, combined with detailed analysis of the backbone dynamics, indicated that the hydrophobic core of this variant is not uniquely structured, but fluctuates on the NMR timescale. The results demonstrate that though much of the native-like secondary structure of Im7 is present in the variants, their hydrophobic cores remain relatively fluid. The comparison of H3G3/H3G6 and L53AI54A/YY suggests that Tyr55 and/or Tyr56 interact with the three-helix core, leading other residues in this region of the protein to dock with the core as folding progresses. In this respect, the three-helix bundle acts as a template for formation of helix III and the creation of the native fold.     

Ion transport in a model gramicidin channel. Structure and thermodynamics.

The potential of mean force for Na+ and K+ ions as a function of position in the interior of a periodic poly(L,D)-alanine model for the gramicidin beta-helix is calculated with a detailed atomic model and realistic interactions. The calculated free energy barriers are 4.5 kcal/mol for Na+ and 1.0 kcal/mol for K+. A decomposition of the free energy demonstrates that the water molecules make a significant contribution to the free energy of activation. There is an increase in entropy at the transition state associated with greater fluctuations. Analysis reveals that the free energy profile of ions in the periodic channel is controlled not by the large interaction energy involving the ion but rather by the weaker water-water, water-peptide and peptide-peptide hydrogen bond interactions. The interior of the channel retains much of the solvation properties of a liquid in its interactions with the cations. Of particular importance is the flexibility of the helix, which permits it to respond to the presence of an ion in a fluidlike manner. The distortion of the helix is local (limited to a few carbonyls) because the structure is too flexible to transmit a perturbation to large distances. The plasticity of the structure (i.e., the property to deform without generating a large energy stress) appears to be an essential factor in the transport of ions, suggesting that a rigid helix model would be inappropriate.     

Tuning RNA Flexibility with Helix Length and Junction Sequence

The increasing awareness of RNA’s central role in biology calls for a new understanding of how RNAs, like proteins, recognize biological partners. Because RNA is inherently flexible, it assumes a variety of conformations. This conformational flexibility can be a critical aspect of how RNA attracts and binds molecular partners. Structurally, RNA consists of rigid basepaired duplexes, separated by flexible non-basepaired regions. Here, using an RNA system consisting of two short helices, connected by a single-stranded (non-basepaired) junction, we explore the role of helix length and junction sequence in determining the range of conformations available to a model RNA. Single-molecule Förster resonance energy transfer reports on the RNA conformation as a function of either mono- or divalent ion concentration. Electrostatic repulsion between helices dominates at low salt concentration, whereas junction sequence effects determine the conformations at high salt concentration. Near physiological salt concentrations, RNA conformation is sensitive to both helix length and junction sequence, suggesting a means for sensitively tuning RNA conformations.     

Consequences of stabilizing the natively disordered f helix for the folding pathway of apomyoglobin

The F helix region of sperm whale apomyoglobin is disordered, undergoing conformational fluctuations between a folded helical conformation and one or more locally unfolded states. To examine the effects of F helix stabilization on the folding pathway of apomyoglobin, we have introduced mutations to augment intrinsic helical structure in the F helix of the kinetic folding intermediate and to increase its propensity to fold early in the pathway, using predictions based on plots of the average area buried upon folding (AABUF) derived from the primary sequence. Two mutant proteins were prepared: a double mutant, P88K/S92K (F2), and a quadruple mutant, P88K/A90L/S92K/A94L (F4). Whereas the AABUF for F2 predicts that the F helix will not fold early in the pathway, the F helix in F4 shows a significantly increased AABUF and is therefore predicted to fold early. Protection of amide protons by formation of hydrogen-bonded helical structure during the early folding events has been analyzed by pH-pulse labeling. Consistent with the AABUF prediction, many of the F helix residues for F4 are significantly protected in the kinetic intermediate but are not protected in the F2 mutant. F4 folds via a kinetically trapped burst-phase intermediate that contains stabilized secondary structure in the A, B, F, G, and H helix regions. Rapid folding of the F helix stabilizes the central core of the misfolded intermediate and inhibits translocation of the H helix back to its native position, thereby decreasing the overall folding rate.     

Role of SRP19 in assembly of the Archaeoglobus fulgidus signal recognition particle

Previous studies have shown that SRP19 promotes association of the highly conserved signal peptide-binding protein, SRP54, with the signal recognition particle (SRP) RNA in both archaeal and eukaryotic model systems. In vitro characterization of this process is now reported using recombinantly expressed components of SRP from the hyperthermophilic, sulfate-reducing archaeon Archaeoglobus fulgidis. A combination of native gel mobility shift, filter binding, and Ni-NTA agarose bead binding assays were used to determine the binding constants for binary and ternary complexes of SRP proteins and SRP RNA. Archaeal SRP54, unlike eukaryotic homologues, has significant intrinsic affinity for 7S RNA (K(D) approximately 15 nM), making it possible to directly compare particles formed in the presence and absence of SRP19 and thereby assess the precise role of SRP19 in the assembly process. Chemical modification studies using hydroxyl radicals and DEPC identify nonoverlapping primary binding sites for SRP19 and SRP54 corresponding to the tips of helix 6 and helix 8 (SRP19) and the distal loop and asymmetric bulge of helix 8 (SRP54). SRP19 additionally induces conformational changes concentrated in the proximal asymmetric bulge of helix 8. Selected nucleotides in this bulge become modified as a result of SRP19 binding but are subsequently protected from modification by formation of the complete complex with SRP54. Together these results suggest a model for assembly in which bridging the ends of helix 6 and helix 8 by SRP19 induces a long-range structural change to present the proximal bulge in a conformation compatible with high-affinity SRP54 binding.     

On the theory of membrane fusion. The stalk mechanism

Based on literary data, conditions necessary for membrane fusion are discussed. It is proposed that fusion mechanisms should be classified according to the primary act involving a change in the membrane structure. Two principal fusion mechanisms are identified: the stalk mechanism, starting with the appearance of a stalk between approaching membranes, and the adhesion mechanism which involves bilayer reorganization as a result of a tight junction of the membranes. The origin and evolution of the monolayer and bilayer stalks between membranes are analysed. Using the expression for the elastic energy of the stalk it was possible to find the value of the spontaneous curvature of its membrane, Ks, at which the existence of a stalk is in principle possible. It is shown that, within the framework of the stalk mechanism, there exists a possibility of either the formation of a stalk of a finite radius, or complete fusion. The Ks values have been determined at which one of the variants occur. The energy barrier of the hydrophobic interaction and the elastic energy barrier, which have to be overcome by the membranes to form the stalk are analysed. The theoretical analysis of the stalk formation mechanism is supported by experimental data. It has been shown by freeze-fracture electron microscopy that the addition of Ca+2, Mg+2, Mn+2 or Cd+2 to suspensions of egg phosphatidylcholine and cardiolipin (1:1 or 3:1) leads to the formation of numerous intramembrane particles (imp's) and crater-like (stalk) structures.     

Comparison of the human and worm p53 structures suggests a way for enhancing stability

Maintaining the native conformation is essential for the proper function of tumor suppressor protein p53. However, p53 is a low-stability protein that can easily lose its function upon structural perturbations such as those resulting from missense mutations, leading to the development of cancer. Therefore, it is important to develop strategies to design stable p53 which still maintains its normal function. Here, we compare the stabilities of the human and worm p53 core domains using molecular dynamics simulations. We find that the worm p53 is significantly more stable than the human form. Detailed analysis of the structural fluctuations shows that the stability difference lies in the peripheral structural motifs that contrast in their structural features and flexibility. The most dramatic difference in stability originates from loop L1, from the turn between helix H1 and beta-strand S5, and from the turn that connects beta-strands S7 and S8. Structural analysis shows significant differences for these motifs between the two proteins. Loop L1 lacks secondary structure, and the turns between helix H1 and strand S5 and between strands S7 and S8 are much longer in the human form p53. On the basis of these differences, we designed a mutant by shortening the turn between strands S7 and S8 to enhance the stability. Surprisingly, this mutant was very stable when probed by molecular dynamics simulations. In addition, the stabilization was not localized in the turn region. Loop L1 was also significantly stabilized. Our results show that stabilizing peripheral structural motifs can greatly enhance the stability of the p53 core domain and therefore is likely to be a viable alternative in the development of stable p53. In addition, loop- or turn-related mutants with different stabilities may also be used to probe the relationship between function, a particular structural motif, and its flexibility.     

Two Arginine Residues Suppress the Flexibility of Nucleosomal DNA in the Canonical Nucleosome Core

The dynamics of nucleosomes containing either canonical H3 or its centromere-specific variant CENP-A were investigated using molecular dynamics simulations. The simulations showed that the histone cores were structurally stable during simulation periods of 100 ns and 50 ns, while DNA was highly flexible at the entry and exit regions and partially dissociated from the histone core. In particular, approximately 20–25 bp of DNA at the entry and exit regions of the CENP-A nucleosome exhibited larger fluctuations than DNA at the entry and exit regions of the H3 nucleosome. Our detailed analysis clarified that this difference in dynamics was attributable to a difference in two basic amino acids in the αN helix; two arginine (Arg) residues in H3 were substituted by lysine (Lys) residues at the corresponding sites in CENP-A. The difference in the ability to form hydrogen bonds with DNA of these two residues regulated the flexibility of nucleosomal DNA at the entry and exit regions. Our exonuclease III assay consistently revealed that replacement of these two Arg residues in the H3 nucleosome by Lys enhanced endonuclease susceptibility, suggesting that the DNA ends of the CENP-A nucleosome are more flexible than those of the H3 nucleosome. This difference in the dynamics between the two types of nucleosomes may be important for forming higher order structures in different phases.     

On the structure of the stator of the mitochondrial ATP synthase

The structure of most of the peripheral stalk, or stator, of the F-ATPase from bovine mitochondria, determined at 2.8 A resolution, contains residues 79-183, 3-123 and 5-70 of subunits b, d and F6, respectively. It consists of a continuous curved alpha-helix about 160 A long in the single b-subunit, augmented by the predominantly alpha-helical d- and F6-subunits. The structure occupies most of the peripheral stalk in a low-resolution structure of the F-ATPase. The long helix in subunit b extends from near to the top of the F1 domain to the surface of the membrane domain, and it probably continues unbroken across the membrane. Its uppermost region interacts with the oligomycin sensitivity conferral protein, bound to the N-terminal region of one alpha-subunit in the F1 domain. Various features suggest that the peripheral stalk is probably rigid rather than resembling a flexible rope. It remains unclear whether the transient storage of energy required by the rotary mechanism takes place in the central stalk or in the peripheral stalk or in both domains.