83 research outputs found

    Model of Dust Thermal Emission of Comet 67p-Churyumov-Gerasimenko for the Rosetta-MIRO Instrument

    Get PDF
    The ESA's Rosetta spacecraft will arrive at comet 67P/Churyumov-Gerasimenko in 2014. The study of gas and dust emission is primary objective of several instruments on the Rosetta spacecraft, including the Microwave Instrument for the Rosetta Orbiter (MIRO). We developed a model of dust thermal emission to estimate the detectability of dust in the vicinity of the nucleus with MIRO. Our model computes the power received by the MIRO antenna in limb viewing as a function of the geometry of the observations and the physical properties of the grains. We show that detection in the millimeter and submillimeter channels can be achieved near perihelion

    Model for the architecture of caveolae based on a flexible, net-like assembly of Cavin1 and Caveolin discs.

    Get PDF
    Caveolae are invaginated plasma membrane domains involved in mechanosensing, signaling, endocytosis, and membrane homeostasis. Oligomers of membrane-embedded caveolins and peripherally attached cavins form the caveolar coat whose structure has remained elusive. Here, purified Cavin1 60S complexes were analyzed structurally in solution and after liposome reconstitution by electron cryotomography. Cavin1 adopted a flexible, net-like protein mesh able to form polyhedral lattices on phosphatidylserine-containing vesicles. Mutating the two coiled-coil domains in Cavin1 revealed that they mediate distinct assembly steps during 60S complex formation. The organization of the cavin coat corresponded to a polyhedral nano-net held together by coiled-coil segments. Positive residues around the C-terminal coiled-coil domain were required for membrane binding. Purified caveolin 8S oligomers assumed disc-shaped arrangements of sizes that are consistent with the discs occupying the faces in the caveolar polyhedra. Polygonal caveolar membrane profiles were revealed in tomograms of native caveolae inside cells. We propose a model with a regular dodecahedron as structural basis for the caveolae architecture

    Orthoparamyxovirinae C Proteins Have a Common Origin and a Common Structural Organization

    Get PDF
    The protein C is a small viral protein encoded in an overlapping frame of the P gene in the subfamily Orthoparamyxovirinae. This protein, expressed by alternative translation initiation, is a virulence factor that regulates viral transcription, replication, and production of defective interfering RNA, interferes with the host-cell innate immunity systems and supports the assembly of viral particles and budding. We expressed and purified full-length and an N-terminally truncated C protein from Tupaia paramyxovirus (TupV) C protein (genus Narmovirus). We solved the crystal structure of the C-terminal part of TupV C protein at a resolution of 2.4 Å and found that it is structurally similar to Sendai virus C protein, suggesting that despite undetectable sequence conservation, these proteins are homologous. We characterized both truncated and full-length proteins by SEC-MALLS and SEC-SAXS and described their solution structures by ensemble models. We established a mini-replicon assay for the related Nipah virus (NiV) and showed that TupV C inhibited the expression of NiV minigenome in a concentration-dependent manner as efficiently as the NiV C protein. A previous study found that the Orthoparamyxovirinae C proteins form two clusters without detectable sequence similarity, raising the question of whether they were homologous or instead had originated independently. Since TupV C and SeV C are representatives of these two clusters, our discovery that they have a similar structure indicates that all Orthoparamyxovirine C proteins are homologous. Our results also imply that, strikingly, a STAT1-binding site is encoded by exactly the same RNA region of the P/C gene across Paramyxovirinae, but in different reading frames (P or C), depending on which cluster they belong to.French Agence Nationale de la RechercheFond de la Recherche MĂ©dicale (FRM)Grenoble Instruct-ERIC centerFRISBIUniversity Grenoble Alpes graduate school (Ecoles Universitaires de Recherche)Peer Reviewe

    Investigating the correlations between water coma emissions and active regions in comet 67P/ Churyumov-Gerasimenko

    Get PDF
    Vibrational emission lines of H2O and CO2 at 2.67 and 4.27 ÎŒm, respectively, were identified by the VIRTIS spectrometer (BockelĂ©e-Morvan et al., 2015; Migliorini et al., 2016; Fink et al., 2016) and mapped from the surface up to about 10 km altitude with a spatial resolution on the order of tens of meters per pixel (Migliorini et al., 2016).Data acquired in April 2015 with the VIRTIS spectrometer on board the Rosetta mission, provided information on the possible correlation between the H2O emission in the inner coma and the exposed water deposits detected in the Hapi region on the 67P/Churyumov-Gerasimenko surface (Migliorini et al., 2106; De Sanctis et al., 2015). Further bright spots attributed to exposed water ice have been identified in other regions by OSIRIS at visible wavelengths (Pommerol, et al., 2015) and confirmed in the infrared by VIRTIS-M in the Imothep region (Filacchione et al., 2016). The small dimensions of these icy spots - approximately 100x100 m (Filacchione et al., 2016) - and the relatively small amount of water ice (about 5%) make uncertain the correlation with the strong emissions in the coma.However, VIRTIS data show that the distribution of jet-like emissions seems to follow the distribution of cliffs and exposed areas identified in the North hemisphere with OSIRIS camera (Vincent et al., 2015). These areas are mainly concentrated in correspondence of comet's rough terrains, while a lack of active regions is observed in the comet's neck. Nevertheless, strong H2O emission is observed above the neck with VIRTIS. This might be a consequence of gas jets that are originated in the surrounding of the neck but converging towards the neck itself. This gaseous activity is the main driver of the dust upwelling (Migliorini et al, 2016; Rinaldi et al., in preparation)In this paper, we investigate the relationship between H2O vapour observed with VIRTIS within 5 km from the 67P/C-G nucleus and the exposed regions identified by OSIRIS on the surface (in the timeframe March to April 2015) with an attempt to address possible variations with the heliocentric distance

    Relationship between inner coma water emissions and ice deposits in comet 67P/Churyumov-Gerasimenko

    Get PDF
    Data acquired in April 2015 with the VIRTIS spectrometer on board the Rosetta mission provided information on the possible correlation between the H2O emission in the inner coma and the exposed water deposits detected in the Hapi region on the 67P/Churyumov-Gerasimenko surface (Migliorini et al. submitted). Further bright spots attributed to exposed water ice have been identified in other regions by OSIRIS at visible wavelengths (Pommerol, et al., 2015) and confirmed in the infrared by VIRTIS-M in the Imothep region (Filacchione et al., 2016). Furthermore, new water ice deposits have been identified in regions located both at the equator and at southern latitudes. These regions might be localised sources of water emissions in the inner coma of 67P/C-G. The present investigation seeks to identify the spatial and temporal correlations between the H2O emissions in the inner coma and the water ice rich deposits on the surface in order to identify the mechanisms operating at the surface-coma interface. It extends the study already carried out for a limited region located in the comet's neck, and identifies how the observed emissions and deposits evolve with the heliocentric distance, as observed by VIRTIS during the Rosetta escort phase mission

    Mapping of thermal properties of comet 67P/C-G and temporal variations

    Get PDF
    The long-term evolution of the surfaces of comets depends mainly on the erosion rate that is driven by the thermal properties of the regolith and the sub-surface material. Following the diurnal and the seasonal thermal cycles, dust and gas are released progressively, increasing the erosion process. The amount of dust released depends on the surface and subsurface temperatures and thus on thermal inertia and bulk composition.The ESA's Rosetta spacecraft has followed the comet 67P/Churyumov-Gerasimenko over several months from 4 AU to 1.28 AU heliocentric distance, and the VIRTIS/Rosetta imaging infrared spectrometer was capable of detecting the thermal emission of the surface longward of 3 microns.The surface temperature was mapped over a large fraction of the nucleus and was previously used to derive thermal inertia of the main geomorphological units.In this presentation, we now focus on two different aspects: (1) We aim to present a complete detailed map of the thermal inertia by combining measurements of similar areas obtained at different viewing angles ; and (2) we track the evolution of the local thermal properties derived over months when the comet was moving towards perihelion. We then discuss and compare our results with the textural features observed at the surface

    Photometric correction for VIRTIS-M data of comet 67P/CG

    Get PDF
    VIRTIS, the Visible Infrared Thermal Imaging Spectrometer onboard the Rosetta orbiter [1], has acquired so far millions of spectra of the comet 67P/Churyumov-Gerasimenko [2]. The instrument is composed of two subsystems: a high-resolution channel (VIRTIS-H) which is a punctual spectrometer (2.0-5-0 ”m) and the mapper (VIRTIS-M) able to produce hyper-spectral images of the target (0.25-5.1 ”m). The huge amount of data produced by VIRTIS has been acquired under different observation and illumination conditions. This induces photometric effects on the measured signal that need to be quantified and removed, in order to characterize the intrinsic spectral variability of the surface. To achieve this task we computed a photometric correction from VIRTIS-M data (Ciarniello et al, 2015), starting from August 2014, when the nucleus was largely resolved (MTP006-MT007 observation sequences) by means of a simplified Hapke model [3]. The global surface single particle phase function (SPPF) and the single scattering albedo (SSA) are determined as well as the effect of sub-pixel roughness is discussed. Comparisons with photometric properties of other comets are shown. This work is supported by the Italian Space Agency (ASI. We acknowledge funding from French and German space agency. References 1- Coradini et al, SSR, 2007 2- Capaccioni et al., Science, in Press, 2015 3- Hapke, Theory of reflectance and emittance spectroscopy. Cambridge University Press, 2012 <P /

    Etudes biophysiques et structurales du complexe de réplication des Rhabdoviridae: La phosphoprotéine et ses interactions avec la nucléoprotéine

    No full text
    Vesicular Stomatitis Virus (VSV) and Rabies Virus (RV) belong to the Rhabdoviridae family and are prototypic members of the genus Vesiculovirus and Lyssavirus, respectively. VSV and RV are envelopped, single stranded, negative sense RNA viruses, and their genome encode successively for five viral proteins including nucleoprotein (N) and phosphoprotein (P), which form, together with the viral RNA dependent RNA polymerase (L), the Rhabdoviridae transcription and replication complex. The aim of this work was to obtain structural information regarding the structure of phosphoprotein and of several of its fragments, free or in complex with N, in order to better understand the mechanisms involved in viral replication. The P protein interacts with N by forming two distinct types of complexes : the N-ARN-P complex results from the association of P with the N-RNA complex, which constitutes the active template for transcription and replication ; the N0-P complex arises from the attachment of P to a N0 molecule, thus preventing binding to non specific RNA and allowing for the specific encapsidation of newly synthesized genomes and antigenomes during viral replication. The data presented here reveals the modular organization of P dimers and highlights the intrinsically disordered character of its N-terminal region involved in N0 binding (PNTD). It is shown that the C-terminal domain of P (PCTD) is an autonomous folding unit that can bind to N-RNA complexes. The atomic scale modeling of P in solution shows that the protein behaves as a partially disordered, highly flexible multidomain protein. Additionally, we constructed a structural model of the interaction between N-RNA and P in silico, which was validated experimentally, and we solved the crystal structure of the N0-PNTD complex using X-Ray diffraction. The work presented here concerning the structure of P, free or in complex with N enhances our understanding of the role of P in the viral replication complex, and emphasizes the importance of structural disorder and conformational changes in the molecular recognition processes involving N and P. The structural models for the N-ARN-P and N0-P complexes also represent attractive new targets for the development of antiviral drugs.Le virus de la stomatite vĂ©siculaire (VSV) et le virus de la rage (RV) appartiennent Ă  la famille des Rhabdoviridae et sont les reprĂ©sentants prototypiques respectifs des genres Vesiculovirus et Lyssavirus. Ces virus sont enveloppĂ©s, et leur gĂ©nome est composĂ© d’une molĂ©cule d’ARN de polaritĂ© nĂ©gative qui encode successivement cinq protĂ©ines virales dont la nuclĂ©oprotĂ©ine (N) et la phosphoprotĂ©ine (P), qui forment, avec l’ARN polymĂ©rase ARN dĂ©pendante virale (L), le complexe de transcription et de rĂ©plication des Rhabdoviridae. L’objectif de mon travail de thĂšse consistait Ă  obtenir des informations structurales concernant la phosphoprotĂ©ine et plusieurs de ses fragments, Ă  l’état libre en solution, ou en complexe avec N, et ce afin de mieux comprendre les mĂ©canismes impliquĂ©s dans la multiplication virale. La protĂ©ine P interagit avec N en formant deux types de complexes distincts : le complexe N-ARN-P, rĂ©sultant de l’association de P avec les complexes N-ARN, qui constituent la matrice utilisĂ©e pour la transcription et la rĂ©plication virale, et le complexe N0-P, qui correspond Ă  la fixation par P d’une molĂ©cule de nuclĂ©oprotĂ©ine N0 monomĂ©rique, empĂȘchant ainsi la fixation non spĂ©cifique de N Ă  l’ARN et permettant l’encapsidation des gĂ©nomes et anti-gĂ©nomes nĂ©o-synthĂ©tisĂ©s lors de la rĂ©plication virale. Les travaux rĂ©alisĂ©s ont permis de mettre en Ă©vidence la nature modulaire des dimĂšres de phosphoprotĂ©ine, et de caractĂ©riser la rĂ©gion N-terminale intrinsĂšquement dĂ©sordonnĂ©e de P (PNTD) impliquĂ©e dans la fixation Ă  N0. Nous avons montrĂ© que le domaine C-terminal impliquĂ© dans la fixation Ă  N-ARN (PCTD) constituait un module structural indĂ©pendant, et modĂ©lisĂ© Ă  l’échelle atomique la structure multi-domaine partiellement dĂ©sordonnĂ©e de P en solution. Nous avons Ă©galement construit un modĂšle atomique in silico de l’interaction entre N-ARN et P, validĂ© expĂ©rimentalement, et enfin rĂ©solus par diffraction des rayons X la structure du complexe N0-PNTD Ă  l’état cristallin. Les travaux prĂ©sentĂ©s concernant la structure de la phosphoprotĂ©ine libre ou en complexe avec la nuclĂ©oprotĂ©ine permettent de mieux comprendre le rĂŽle de P dans le complexe de rĂ©plication, et soulignent l’importance du dĂ©sordre molĂ©culaire et des changements conformationnels dans les processus de reconnaissance molĂ©culaire impliquant N et P. Les modĂšles structuraux des complexes N-ARN-P et N0-P constituent par ailleurs des nouvelles cibles intĂ©ressantes pour le dĂ©veloppement de composĂ©s antiviraux

    Propriétés physiques des anneaux de Saturne : de CAMIRAS à la mission CASSINI.

    Get PDF
    This thesis presents a study of the rotational properties of particles in Saturn's A and C rings. The own rotation of particles is a dynamical key parameter which plays a role during mutual collisions. The distribution of the spin rate w depends indeed on relative speeds but also on the surface quality of regolith (porosity and roughness) and thus on the internal structure of particles. To constrain w, we need to interpret the thermal emission (function of thermal inertia Tau and w) of the disc according to the phase angle and the planetocentric longitude, as it is still impossible to observe particles separately. Azimuthal variations of temperature observed with various phases angles are modulated by the cooling of the particles, when they cross the shadow of the planet. The heating and cooling rates make it possible to measure thermal inertia, whereas the differences in temperature with the phase angle inform us on the anisotropy of emission associated with the spin rate. Azimuthal variations of temperature were observed in the mid-infrared, at weak phase angle with imagers CAMIRAS (CFHT) and VISIR (VLT), and at multiple phases angles with IRIS (Voyager) and CIRS (Cassini) spectrometers, offering respectively a total or partial azimuthal coverage. A thermal model of planetary ring made up of icy spherical particles in rotation and distributed according to a monolayer structure was developed to interpret the observed temperatures. It enables us to determine how the temperature of the disc, submitted to the multiple sources of heating (Sun, Saturn... etc), varies with the phase angle and the longitude according to the thermal properties of particles. The significant asymmetrycal emission to weak or strong phase shows that the largest particles, which contain a significant fraction of the C ring mass, have an average spin rate w/Omega =0.5±0.4.This result, obtained with the assumptions of a mono size distribution and a monolayer vertical structure, is compatible with results of dynamical simulations. The thermal inertia of the regolith in the C ring (Tau = 6.0 ± 4Jm-2K-1s-1/2) is 3 orders of magnitude weaker than that of the crystalline water ice, and confirms a very porous structure, probably generated by cracks on the surface of the particles. They are probably the consequence of the permanent patching due to the mutual collisions, or the forces of tensions related to the signi- ficant variations in temperature with each orbit. In addition to azimuthal variations in temperature of the A ring, related to the spin rate and the cooling of particles in the Saturn's shadow, a modulation of brightness temperature, correlated with variations of optical depth, is put. This variation could be highlighted by the observations of CIRS at multiple phases and is explained by the presence of gravitational instabilities known under the name of "wakes". The thermal emission of the A ring observed with VISIR, after the taking into account of CIRS observations, is similar to that coming from plane structures in which the particles form aggregates. The high angular resolution accessible with the VLT enabled us, for the first time, to measure the azimuthal variations of temperature in this ring and to deduce its thermal inertia from it. The found value (Tau = 4±3Jm-2K-1s-1/2), under the assumption of a monolayer plane structure, is virtually identical to that of the rings C and B, indicating a probably similar surface quality.Cette thĂšse prĂ©sente une Ă©tude des propriĂ©tĂ©s rotationnelles des particules dans les anneaux A et C de Saturne. La rotation des particules sur elles mĂȘmes est un des paramĂštres dynamiques clĂ© qui entre en jeu au cours des collisions mutuelles. La distribution du spin w dĂ©pend en effet des vitesses relatives mais aussi de l'Ă©tat de surface du rĂ©golite (porositĂ© et rugositĂ©) et donc de la structure interne des particules. La contrainte de w passe par l'interprĂ©tation de l'Ă©mission thermique (fonction de l'inertie thermique Tau et de w) du disque en fonction de l'angle de phase et de la longitude planĂ©tocentrique, car il n'est pas encore possible d'observer les particules individuellement. Les variations azimutales de tempĂ©rature observĂ©es Ă  diffĂ©rents angles de phase sont modulĂ©es par le refroidissement des particules Ă  chaque orbite, lorsqu'elles traversent l'ombre de la planĂšte. Les vitesses de rĂ©chauffement et de refroidissement permettent de mesurer l'inertie thermique, alors que les diffĂ©rences de tempĂ©rature en fonction de l'angle de phase nous informent sur l'anisotropie d'Ă©mission associĂ©e au spin.Ces variations de tempĂ©rature ont Ă©tĂ© observĂ©es dans l'infrarouge, Ă  faible angle de phase avec les camĂ©ras CAMIRAS (CFHT) et VISIR (VLT), et Ă  de multiples angles de phase avec les spectromĂštres IRIS (Voyager) et CIRS (Cassini), offrant respectivement une couverture azimutale totale ou partielle. Un modĂšle thermique d'anneau planĂ©taire constituĂ© de particules de glace sphĂ©riques en rotation et rĂ©parties suivant une structure monocouche a Ă©tĂ© dĂ©veloppĂ© pour interprĂ©ter les tempĂ©ratures observĂ©es. Il permet de dĂ©terminer comment la tempĂ©rature du disque, soumis aux multiples sources de chauffage (Soleil, Saturne...etc), varie avec l'angle de phase et la longitude en fonction des propriĂ©tĂ©s thermiques des particules.L'importante asymĂ©trie d'Ă©mission Ă  faible ou fort angle de phase montre que les plus grosses particules, qui contiennent une fraction importante de la masse de l'anneau C, ont une vitesse moyenne de rotation proche de la rotation Keplerienne Omega(w/Omega =0.5±0.4). Ce rĂ©sultat, obtenu avec les hypothĂšses d'une distribution mono taille des particules, et suivant une structure monocouche, est compatible avec les rĂ©sultats des simulations dynamiques. L'inertie thermique du rĂ©golite de l'anneau C (Tau = 6.0 ± 4Jm-2K-1s-1/2) est 3 ordres de grandeur plus faible que celle de la glace d'eau cristalline, et confirme une structure trĂšs poreuse, probablement engendrĂ©e par des fissures Ă  la surface des particules. Elles sont probablement la consĂ©quence du resurfaçage permanent dĂ» aux collisions mutuelles, ou aux forces de tensions liĂ©es aux importantes variations de tempĂ©rature Ă  chaque orbite.Aux variations de tempĂ©rature azimutales de l'anneau A liĂ©es au spin et au refroidissement des particules dans l'ombre de la planĂšte, s'ajoute une modulation de tempĂ©rature de brillance, corrĂ©lĂ©e avec la variation de profondeur optique. Cette variation a pu ĂȘtre mise en Ă©vidence par les observations de CIRS Ă  de multiples angles de phase et s'explique par la prĂ©sence d'instabilit Ă©s gravitationnelles connues sous le nom de " wakes ". L'Ă©mission thermique de l'anneau A observĂ©e avec VISIR, aprĂšs la prise en compte des observations de CIRS, est similaire Ă  celle provenant de structures planes dans lesquelles les particules forment des agrĂ©gats. La haute rĂ©solution angulaire accessible au VLT nous a permis, pour la premiĂšre fois, de mesurer les variations azimutales de tempĂ©rature dans cette rĂ©gion et d'en dĂ©duire son inertie thermique. La valeur trouvĂ©e (Tau = 4 ± 3Jm-2K-1s-1/2), sous l'hypothĂšse d'une structure plane monocouche, est sensiblement identique Ă  celle des anneaux C et B, indiquant un Ă©tat de surface probablement similaire

    Probing Pluto’s underworld: Ice temperatures from microwave radiometry decoupled from surface conditions

    No full text
    International audiencePresent models admit a wide range of 2015 surface conditions at Pluto and Charon, where the atmospheric pressure may undergo dramatic seasonal variation and for which measurements are imminent from the New Horizons mission. One anticipated observation is the microwave brightness temperature, heretofore anticipated as indicating surface conditions relevant to surface-atmosphere equilibrium. However, drawing on recent experience with Cassini observations at Iapetus and Titan, we call attention to the large electrical skin depth of outer solar system materials such as methane, nitrogen or water ice, such that this observation may indicate temperatures averaged over depths of several or tens of meters beneath the surface. Using a seasonally-forced thermal model to determine microwave emission we predict that the southern hemisphere observations (in polar night) of New Horizons in July 2015 will suggest effective temperatures of ∌40 K, reflecting deep heat buried over the last century of summer, even if the atmospheric pressure suggests that the surface nitrogen frost point may be much lower
    • 

    corecore