1000 resultados para Protein Loops


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Pyrin domain (PYD)-containing proteins are key components of pathways that regulate inflammation, apoptosis, and cytokine processing. Their importance is further evidenced by the consequences of mutations in these proteins that give rise to autoimmune and hyperinflammatory syndromes. PYDs, like other members of the death domain ( DD) superfamily, are postulated to mediate homotypic interactions that assemble and regulate the activity of signaling complexes. However, PYDs are presently the least well characterized of all four DD subfamilies. Here we report the three-dimensional structure and dynamic properties of ASC2, a PYD-only protein that functions as a modulator of multidomain PYD-containing proteins involved in NF-KB and caspase-1 activation. ASC2 adopts a six-helix bundle structure with a prominent loop, comprising 13 amino acid residues, between helices two and three. This loop represents a divergent feature of PYDs from other domains with the DD fold. Detailed analysis of backbone N-15 NMR relaxation data using both the Lipari-Szabo model-free and reduced spectral density function formalisms revealed no evidence of contiguous stretches of polypeptide chain with dramatically increased internal motion, except at the extreme N and C termini. Some mobility in the fast, picosecond to nanosecond timescale, was seen in helix 3 and the preceding alpha 2-alpha 3 loop, in stark contrast to the complete disorder seen in the corresponding region of the NALP1 PYD. Our results suggest that extensive conformational flexibility in helix 3 and the alpha 2-alpha 3 loop is not a general feature of pyrin domains. Further, a transition from complete disorder to order of the alpha 2-alpha 3 loop upon binding, as suggested for NALP1, is unlikely to be a common attribute of pyrin domain interactions.

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The pores of voltage-gated ion channels are lined by protein loops that determine selectivity and conductance. The relative orientations of these "P" loops remain uncertain, as do the distances between them. Using site-directed mutagenesis, we introduced pairs of cysteines into the P loops of micro1 rat skeletal muscle sodium channels and sought functional evidence of proximity between the substituted residues. Only cysteinyl residues that are in close proximity can form disulfide bonds or metal-chelating sites. The mutant Y401C (domain I) spontaneously formed a disulfide bond when paired with E758C in the P loop of domain II; the same residue, when coupled with G1530C in domain IV, created a high-affinity binding site for Cd2+ ions. The results provide the first specific constraints for intramolecular dimensions of the sodium channel pore.

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We describe the mechanism of ribonuclease inhibition by ribonuclease inhibitor, a protein built of leucine-rich repeats, based on the crystal structure of the complex between the inhibitor and ribonuclease A. The structure was determined by molecular replacement and refined to an R(cryst) of 19.4% at 2.5 Angstrom resolution. Ribonuclease A binds to the concave region of the inhibitor protein comprising its parallel beta-sheet and loops. The inhibitor covers the ribonuclease active site and directly contacts several active-site residues. The inhibitor only partially mimics the RNase-nucleotide interaction and does not utilize the pi phosphate-binding pocket of ribonuclease A, where a sulfate ion remains bound. The 2550 Angstrom(2) of accessible surface area buried upon complex formation may be one of the major contributors to the extremely tight association (K-i = 5.9 x 10(-14) M). The interaction is predominantly electrostatic; there is a high chemical complementarity with 18 putative hydrogen bonds and salt links, but the shape complementarity is lower than in most other protein-protein complexes. Ribonuclease inhibitor changes its conformation upon complex formation; the conformational change is unusual in that it is a plastic reorganization of the entire structure without any obvious hinge and reflects the conformational flexibility of the structure of the inhibitor. There is a good agreement between the crystal structure and other biochemical studies of the interaction. The structure suggests that the conformational flexibility of RI and an unusually large contact area that compensates for a lower degree of complementarity may be the principal reasons for the ability of RI to potently inhibit diverse ribonucleases. However, the inhibition is lost with amphibian ribonucleases that have substituted most residues corresponding to inhibitor-binding residues in RNase A, and with bovine seminal ribonuclease that prevents inhibitor binding by forming a dimer. (C) 1996 Academic Press Limited

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This work compares the structural/dynamics features of the wild-type alb-adrenergic receptor (AR) with those of the D142A active mutant and the agonist-bound state. The two active receptor forms were compared in their isolated states as well as in their ability to form homodimers and to recognize the G alpha q beta 1 gamma 2 heterotrimer. The analysis of the isolated structures revealed that, although the mutation- and agonist-induced active states of the alpha 1b-AR are different, they, however, share several structural peculiarities including (a) the release of some constraining interactions found in the wild-type receptor and (b) the opening of a cytosolic crevice formed by the second and third intracellular loops and the cytosolic extensions of helices 5 and 6. Accordingly, also their tendency to form homodimers shows commonalties and differences. In fact, in both the active receptor forms, helix 6 plays a crucial role in mediating homodimerization. However, the homodimeric models result from different interhelical assemblies. On the same line of evidence, in both of the active receptor forms, the cytosolic opened crevice recognizes similar domains on the G protein. However, the docking solutions are differently populated and the receptor-G protein preorientation models suggest that the final complexes should be characterized by different interaction patterns.

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This study proposes a theoretical model describing the electrostatically driven step of the alpha 1 b-adrenergic receptor (AR)-G protein recognition. The comparative analysis of the structural-dynamics features of functionally different receptor forms, i.e., the wild type (ground state) and its constitutively active mutants D142A and A293E, was instrumental to gain insight on the receptor-G protein electrostatic and steric complementarity. Rigid body docking simulations between the different forms of the alpha 1 b-AR and the heterotrimeric G alpha q, G alpha s, G alpha i1, and G alpha t suggest that the cytosolic crevice shared by the active receptor and including the second and the third intracellular loops as well as the cytosolic extension of helices 5 and 6, represents the receptor surface with docking complementarity with the G protein. On the other hand, the G protein solvent-exposed portions that recognize the intracellular loops of the activated receptors are the N-terminal portion of alpha 3, alpha G, the alpha G/alpha 4 loop, alpha 4, the alpha 4/beta 6 loop, alpha 5, and the C-terminus. Docking simulations suggest that the two constitutively active mutants D142A and A293E recognize different G proteins with similar selectivity orders, i.e., G alpha q approximately equal to G alpha s > G alpha i > G alpha t. The theoretical models herein proposed might provide useful suggestions for new experiments aiming at exploring the receptor-G protein interface.

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BACKGROUND: The nuclear receptors are a large family of eukaryotic transcription factors that constitute major pharmacological targets. They exert their combinatorial control through homotypic heterodimerisation. Elucidation of this dimerisation network is vital in order to understand the complex dynamics and potential cross-talk involved. RESULTS: Phylogeny, protein-protein interactions, protein-DNA interactions and gene expression data have been integrated to provide a comprehensive and up-to-date description of the topology and properties of the nuclear receptor interaction network in humans. We discriminate between DNA-binding and non-DNA-binding dimers, and provide a comprehensive interaction map, that identifies potential cross-talk between the various pathways of nuclear receptors. CONCLUSION: We infer that the topology of this network is hub-based, and much more connected than previously thought. The hub-based topology of the network and the wide tissue expression pattern of NRs create a highly competitive environment for the common heterodimerising partners. Furthermore, a significant number of negative feedback loops is present, with the hub protein SHP [NR0B2] playing a major role. We also compare the evolution, topology and properties of the nuclear receptor network with the hub-based dimerisation network of the bHLH transcription factors in order to identify both unique themes and ubiquitous properties in gene regulation. In terms of methodology, we conclude that such a comprehensive picture can only be assembled by semi-automated text-mining, manual curation and integration of data from various sources.

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Addition of a 50 mM mixture of l-arginine and l-glutamic acid (RE) is extensively used to improve protein solubility and stability, although the origin of the effect is not well understood. We present Small Angle X-ray Scattering (SAXS) and Nuclear Magnetic Resonance (NMR) results showing that RE induces protein compaction by collapsing flexible loops on the protein core. This is suggested to be a general mechanism preventing aggregation and improving resistance to proteases and to originate from the polyelectrolyte nature of RE. Molecular polyelectrolyte mixtures are expected to display long range correlation effects according to dressed interaction site theory. We hypothesize that perturbation of the RE solution by dissolved proteins is proportional to the volume occupied by the protein. As a consequence, loop collapse, minimizing the effective protein volume, is favored in the presence of RE.

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Des variations importantes du surenroulement de l’ADN peuvent être générées durant la phase d’élongation de la transcription selon le modèle du « twin supercoiled domain ». Selon ce modèle, le déplacement du complexe de transcription génère du surenroulement positif à l’avant, et du surenroulement négatif à l’arrière de l’ARN polymérase. Le rôle essentiel de la topoisomérase I chez Escherichia coli est de prévenir l’accumulation de ce surenroulement négatif générée durant la transcription. En absence de topoisomérase I, l’accumulation de ce surenroulement négatif favorise la formation de R-loops qui ont pour conséquence d’inhiber la croissance bactérienne. Les R-loops sont des hybrides ARN-ADN qui se forment entre l’ARN nouvellement synthétisé et le simple brin d’ADN complémentaire. Dans les cellules déficientes en topoisomérase I, des mutations compensatoires s’accumulent dans les gènes qui codent pour la gyrase, réduisant le niveau de surenroulement négatif du chromosome et favorisant la croissance. Une des ces mutations est une gyrase thermosensible qui s’exprime à 37 °C. La RNase HI, une enzyme qui dégrade la partie ARN d’un R-loop, peut aussi restaurer la croissance en absence de topoisomérase I lorsqu’elle est produite en très grande quantité par rapport à sa concentration physiologique. En présence de topoisomérase I, des R-loops peuvent aussi se former lorsque la RNase HI est inactive. Dans ces souches mutantes, les R-loops induisent la réponse SOS et la réplication constitutive de l’ADN (cSDR). Dans notre étude, nous montrons comment les R-loops formés en absence de topoisomérase I ou RNase HI peuvent affecter négativement la croissance des cellules. Lorsque la topoisomérase I est inactivée, l’accumulation d’hypersurenroulement négatif conduit à la formation de nombreux R-loops, ce qui déclenche la dégradation de l’ARN synthétisé. Issus de la dégradation de l’ARNm de pleine longueur, des ARNm incomplets et traductibles s’accumulent et causent l’inhibition de la synthèse protéique et de la croissance. Le processus par lequel l’ARN est dégradé n’est pas encore complètement élucidé, mais nos résultats soutiennent fortement que la RNase HI présente en concentration physiologique est responsable de ce phénotype. Chose importante, la RNase E qui est l’endoribonuclease majeure de la cellule n’est pas impliquée dans ce processus, et la dégradation de l’ARN survient avant son action. Nous montrons aussi qu’une corrélation parfaite existe entre la concentration de RNase HI, l’accumulation d’hypersurenroulement négatif et l’inhibition de la croissance bactérienne. Lorsque la RNase HI est en excès, l’accumulation de surenroulement négatif est inhibée et la croissance n’est pas affectée. L’inverse se produit Lorsque la RNase HI est en concentration physiologique. En limitant l’accumulation d’hypersurenroulement négatif, la surproduction de la RNase HI prévient alors la dégradation de l’ARN et permet la croissance. Quand la RNase HI est inactivée en présence de topoisomérase I, les R-loops réduisent le niveau d’expression de nombreux gènes, incluant des gènes de résistance aux stress comme rpoH et grpE. Cette inhibition de l’expression génique n’est pas accompagnée de la dégradation de l’ARN contrairement à ce qui se produit en absence de topoisomérase I. Dans le mutant déficient en RNase HI, la diminution de l’expression génique réduit la concentration cellulaire de différentes protéines, ce qui altère négativement le taux de croissance et affecte dramatiquement la survie des cellules exposées aux stress de hautes températures et oxydatifs. Une inactivation de RecA, le facteur essentiel qui déclenche la réponse SOS et le cSDR, ne restaure pas l’expression génique. Ceci démontre que la réponse SOS et le cSDR ne sont pas impliqués dans l’inhibition de l’expression génique en absence de RNase HI. La croissance bactérienne qui est inhibée en absence de topoisomérase I, reprend lorsque l’excès de surenroulement négatif est éliminé. En absence de RNase HI et de topoisomérase I, le surenroulement négatif est très relaxé. Il semble que la réponse cellulaire suite à la formation de R-loops, soit la relaxation du surenroulement négatif. Selon le même principe, des mutations compensatoires dans la gyrase apparaissent en absence de topoisomérase I et réduisent l’accumulation de surenroulement négatif. Ceci supporte fortement l’idée que le surenroulement négatif joue un rôle primordial dans la formation de R-loop. La régulation du surenroulement négatif de l’ADN est donc une tâche essentielle pour la cellule. Elle favorise notamment l’expression génique optimale durant la croissance et l’exposition aux stress, en limitant la formation de R-loops. La topoisomérase I et la RNase HI jouent un rôle important et complémentaire dans ce processus.

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Chez la bactérie Escherichia coli, la topoisomérase I et la gyrase représentent deux topoisomérases majeures qui participent à la régulation du surenroulement de l’ADN. Celles-ci sont codées respectivement par les gènes topA et par gyrA et gyrB. Chez les mutants topA, l’excès de surenroulement négatif qui est généré en amont de la polymérase ARN lors de la phase d’élongation de la transcription de l’ADN, entraine la formation de R-loops. Les R-loops sont des hybrides ARN-ADN qui in vivo sont formés lorsque l’ARN nouvellement transcrit forme un hybride avec le brin d’ADN matrice, le brin d’ADN complémentaire demeurant sous forme simple brin. La RNase HI est une endoribonucléase codée par le gène rnhA. Elle dégrade l’ARN de R-loops, entre autres, pour empêcher l’initiation de la réplication à des sites autres que l’origine normale, oriC. Chez les mutants rnhA, on observe une réplication indépendante de l’origine oriC. Ce type de réplication appelé cSDR, pourrait donc expliquer, du moins en partie, l’inhibition de la croissance de doubles mutants topA rnhA. A l’aide de la mutagenèse au transposon Tn5, il a été possible d’isoler des suppresseurs extragéniques qui permettaient la croissance des doubles mutants topA rnhA. Plusieurs de ces suppresseurs ont le transposon inséré dans le gène codant pour la RNase E, l’endoribonucléase principale impliquée dans la dégradation des ARNms chez E. coli. La majorité des insertions se retrouvent dans la partie C-terminale de la protéine qui est impliquée dans l’assemblage d’un complexe multiprotéique appelé l’ARN dégradosome. Les résultats obtenus démontrent que ces suppresseurs diminuent le cSDR ainsi que la réponse SOS induite constitutivement en l’absence de la RNase HI. Sachant que la RNase HI est une endoribonucléase tout comme la RNase E, une collaboration entre les deux enzymes suggère que la RNase E pourrait également jouer un rôle potentiel dans le contrôle de la formation des R-loops et bien évidemment de leur retrait au sein de la cellule. À l’opposé, il est possible que la RNase HI puisse avoir comme autre fonction la prise en charge de la maturation et de la dégradation des molécules d’ARNs.

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Conserved among all coronaviruses are four structural proteins: the matrix (M), small envelope (E), and spike (S) proteins that are embedded in the viral membrane and the nucleocapsid phosphoprotein (N), which exists in a ribonucleoprotein complex in the lumen. The N-terminal domain of coronaviral N proteins (N-NTD) provides a scaffold for RNA binding, while the C-terminal domain (N-CTD) mainly acts as oligomerization modules during assembly. The C terminus of the N protein anchors it to the viral membrane by associating with M protein. We characterized the structures of N-NTD from severe acute respiratory syndrome coronavirus (SARS-CoV) in two crystal forms, at 1.17 A (monoclinic) and at 1.85 A (cubic), respectively, resolved by molecular replacement using the homologous avian infectious bronchitis virus (IBV) structure. Flexible loops in the solution structure of SARS-CoV N-NTD are now shown to be well ordered around the beta-sheet core. The functionally important positively charged beta-hairpin protrudes out of the core, is oriented similarly to that in the IBV N-NTD, and is involved in crystal packing in the monoclinic form. In the cubic form, the monomers form trimeric units that stack in a helical array. Comparison of crystal packing of SARS-CoV and IBV N-NTDs suggests a common mode of RNA recognition, but they probably associate differently in vivo during the formation of the ribonucleoprotein complex. Electrostatic potential distribution on the surface of homology models of related coronaviral N-NTDs suggests that they use different modes of both RNA recognition and oligomeric assembly, perhaps explaining why their nucleocapsids have different morphologies.

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Virulence in Staphylococcus aureus is regulated via agr-dependent quorum sensing in which an autoinducing peptide (AIP) activates AgrC, a histidine protein kinase. AIPs are usually thiolactones containing seven to nine amino acid residues in which the thiol of the central cysteine is linked to the alpha-carboxyl of the C-terminal amino acid residue. The staphylococcal agr locus has diverged such that the AIPs of the four different S. aureus agr groups self-activate but cross-inhibit. Consequently, although the agr system is conserved among the staphylococci, it has undergone significant evolutionary divergence whereby to retain functionality, any changes in the AIP-encoding gene (agrD) that modifies AIP structure must be accompanied by corresponding changes in the AgrC receptor. Since AIP-1 and AIP-4 only differ by a single amino acid, we compared the transmembrane topology of AgrC1 and AgrC4 to identify amino acid residues involved in AIP recognition. As only two of the three predicted extracellular loops exhibited amino acid differences, site-specific mutagenesis was used to exchange the key AgrC1 and AgrC4 amino acid residues in each loop either singly or in combination. A novel lux-based agrP3 reporter gene fusion was constructed to evaluate the response of the mutated AgrC receptors. The data obtained revealed that while differential recognition of AIP-1 and AIP-4 depends primarily on three amino acid residues in loop 2, loop 1 is essential for receptor activation by the cognate AIP. Furthermore, a single mutation in the AgrC1 loop 2 resulted in conversion of (Ala5)AIP-1 from a potent antagonist to an activator, essentially resulting in the forced evolution of a new AIP group. Taken together, our data indicate that loop 2 constitutes the predicted hydrophobic pocket that binds the AIP thiolactone ring while the exocyclic amino acid tail interacts with loop 1 to facilitate receptor activation.

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The components of many signaling pathways have been identified and there is now a need to conduct quantitative data-rich temporal experiments for systems biology and modeling approaches to better understand pathway dynamics and regulation. Here we present a modified Western blotting method that allows the rapid and reproducible quantification and analysis of hundreds of data points per day on proteins and their phosphorylation state at individual sites. The approach is of particular use where samples show a high degree of sample-to-sample variability such as primary cells from multiple donors. We present a case study on the analysis of >800 phosphorylation data points from three phosphorylation sites in three signaling proteins over multiple time points from platelets isolated from ten donors, demonstrating the technique's potential to determine kinetic and regulatory information from limited cell numbers and to investigate signaling variation within a population. We envisage the approach being of use in the analysis of many cellular processes such as signaling pathway dynamics to identify regulatory feedback loops and the investigation of potential drug/inhibitor responses, using primary cells and tissues, to generate information about how a cell's physiological state changes over time.

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Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

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In this thesis I treat various biophysical questions arising in the context of complexed / ”protein-packed” DNA and DNA in confined geometries (like in viruses or toroidal DNA condensates). Using diverse theoretical methods I consider the statistical mechanics as well as the dynamics of DNA under these conditions. In the first part of the thesis (chapter 2) I derive for the first time the single molecule ”equation of state”, i.e. the force-extension relation of a looped DNA (Eq. 2.94) by using the path integral formalism. Generalizing these results I show that the presence of elastic substructures like loops or deflections caused by anchoring boundary conditions (e.g. at the AFM tip or the mica substrate) gives rise to a significant renormalization of the apparent persistence length as extracted from single molecule experiments (Eqs. 2.39 and 2.98). As I show the experimentally observed apparent persistence length reduction by a factor of 10 or more is naturally explained by this theory. In chapter 3 I theoretically consider the thermal motion of nucleosomes along a DNA template. After an extensive analysis of available experimental data and theoretical modelling of two possible mechanisms I conclude that the ”corkscrew-motion” mechanism most consistently explains this biologically important process. In chapter 4 I demonstrate that DNA-spools (architectures in which DNA circumferentially winds on a cylindrical surface, or onto itself) show a remarkable ”kinetic inertness” that protects them from tension-induced disruption on experimentally and biologically relevant timescales (cf. Fig. 4.1 and Eq. 4.18). I show that the underlying model establishes a connection between the seemingly unrelated and previously unexplained force peaks in single molecule nucleosome and DNA-toroid stretching experiments. Finally in chapter 5 I show that toroidally confined DNA (found in viruses, DNAcondensates or sperm chromatin) undergoes a transition to a twisted, highly entangled state provided that the aspect ratio of the underlying torus crosses a certain critical value (cf. Eq. 5.6 and the phase diagram in Fig. 5.4). The presented mechanism could rationalize several experimental mysteries, ranging from entangled and supercoiled toroids released from virus capsids to the unexpectedly short cholesteric pitch in the (toroidaly wound) sperm chromatin. I propose that the ”topological encapsulation” resulting from our model may have some practical implications for the gene-therapeutic DNA delivery process.