Héliosphère

vignette|upright=1.5|Représentation schématique de l'héliosphère, depuis le système solaire jusqu'à l'espace interstellaire (vue d'artiste). vignette|upright=1.5|Schéma simplifié de l'héliosphère, montrant la position approximative des sondes et 2 en 2005 (NB : l'hypothèse de l'onde de choc au-delà de l'héliopause est aujourd'hui abandonnée). L'héliosphère est l'astrosphère du Soleil, une zone en forme de bulle allongée dans l'espace, engendrée par les vents solaires. Sa limite est l'héliopause, qui délimite la zone d'influence des vents solaires, lorsqu'ils rencontrent le milieu interstellaire. Le vent solaire consiste en la projection de particules atomiques (essentiellement protons et électrons) par la haute atmosphère de notre étoile, le Soleil. Ce plasma impose une pression (une sorte de souffle) vers l'extérieur du système solaire et repousse le flux de particules similaires mais provenant de l'espace lointain. La forme de la bulle ainsi produite n'est que très approximativeme

Superdiffusive transport in laboratory and astrophysical plasmas

Alexandre Dominique Bovet, Ambrogio Fasoli, Ivo Furno, Kyle Gustafson, Paolo Ricci

In the last few years it has been demonstrated, both by data analysis and by numerical simulations, that the transport of energetic particles in the presence of magnetic turbulence can be superdiffusive rather than normal diffusive (Gaussian). The term ‘superdiffusive’ refers to the mean square displacement of particle positions growing superlinearly with time, as compared to the normal linear growth. The so-called anomalous transport, which in general comprises both subdiffusion and superdiffusion, has gained growing attention during the last two decades in many fields including laboratory plasma physics, and recently in astrophysics and space physics. Here we show a number of examples, both from laboratory and from astrophysical plasmas, where superdiffusive transport has been identified, with a focus on what could be the main influence of superdiffusion on fundamental processes like diffusive shock acceleration and heliospheric energetic particle propagation. For laboratory plasmas, superdiffusion appears to be due to the presence of electrostatic turbulence which creates long-range correlations and convoluted structures in perpendicular transport: this corresponds to a similar phenomenon in the propagation of solar energetic particles (SEPs) which leads to SEP dropouts. For the propagation of energetic particles accelerated at interplanetary shocks in the solar wind, parallel superdiffusion seems to be prevailing; this is based on a pitch-angle scattering process different from that envisaged by quasi-linear theory, and this emphasizes the importance of nonlinear interactions and trapping effects. In the case of supernova remnant shocks, parallel superdiffusion is possible at quasi-parallel shocks, as occurring in the interplanetary space, and perpendicular superdiffusion is possible at quasi-perpendicular shocks, as corresponding to Richardson diffusion: therefore, cosmic ray acceleration at supernova remnant shocks should be formulated in terms of superdiffusion. The possible relations among anomalous transport in laboratory, heliospheric, and astrophysical plasmas will be indicated.

Cambridge University Press2015

Superdiffusive transport in laboratory and astrophysical plasmas

Alexandre Dominique Bovet, Ambrogio Fasoli, Ivo Furno, Kyle Gustafson, Paolo Ricci

Cambridge University Press2015

Study of the Modification of the Shock/Boundary Layer Interaction on an Isolated Airfoil by Slot Suction

Superdiffusive transport in laboratory and astrophysical plasmas

On high power circulators with mismatched terminations

Study of the Modification of the Shock/Boundary Layer Interaction on an Isolated Airfoil by Slot Suction

Superdiffusive transport in laboratory and astrophysical plasmas

On high power circulators with mismatched terminations