1,725,267 research outputs found
Bizzarri e la pubblicità: dalla creatività alla cura
No full text“Giulio Bizzarri è una figura difficile da definire in modo univoco. Tutta la sua opera è intesa a scardinare una lettura disciplinare a favore di un gioco di specchi che, attraverso il sistema combinatorio e lo scarto surrealista favorisse una visione sempre rinnovata, e pertanto mai scontata, della realtà. Un processo che lo ha portato a considerare la direzione artistica il mestiere cucito su misura, sempre inteso in termini di ricerca, nella pubblicità e nella comunicazione in ambito culturale così come nella didattica. Un mestiere mai limitato da una tecnica o a un ambito di ricerca che chiedeva piuttosto di aprirsi a un sistema corale di cui lui era l’artefice inventore, l’appartato ricercatore, l’ordinatore perfezionista.” - Dall’introduzione di Marta Sironi, storica dell’arte
Escrituras de la enfermedad y discurso decolonial en la literatura hispanoamericana reciente
Full text linkAbstract
Introducción. Modernidades otras y ‘afectadas’: la enfermedad como nuestra parte de noche, Gabriele Bizzarri p. 211
Paradoja immunitaria, Lina Meruane p. 222
La opresión de la ceguera: mirada, memoria y poder en Sangre en el ojo, de Lina Meruane, Paola Susana Solorza p. 230
Cuerpos infectos: Copi, Perlongher y Evita, Lucía Caminada Rossetti p. 240
Un yo sin yo. Memoria y subjetividad en Desarticulaciones de Sylvia Molloy, Andrea Ostrov p. 257
La enfermedad del susto: identidad y discurso crítico desde los Andes, Paola Mancosu p. 268
El verbo afectar: afectos y discreción en El verbo J de Claudia Hernández, Emanuela Jossa p. 285
En la intersección de fantástico y enfermedad: una lectura de “El Hombre de la Pierna” de Giovanna Rivero y “La respiración cavernaria” de Samanta Schweblin, Anna Boccuti p. 30
Determination of the temperature field due to frictional heating on a sliding interface
No full textIn the recent years we assisted to an increasing number of studies devoted to the quantification of the effects of temperature developed as a consequence of frictional heat on a sliding interface. The temperature field generated on the fault surface is responsible of a large number of physical and chemical dissipative process, summarized in Bizzarri (2010a).
Among these we mention here the flash heating of micro–asperity contacts, basically consisting in a different behavior of fault friction at high fault slip velocities [e.g., Bizzarri, 2009a; Noda et al., 2009], the melting of rocks and gouge particles [Nielsen et al., 2008; Bizzarri, 2010b], the thermally–induced pressurization of fluids in saturated fault structures [Andrews, 2002; Bizzarri and Cocco, 2006; Rice, 2006].
A key issue of all these studies is the proper calculation of the temperature distribution on the fault surface and its temporal evolution.
In this study we compare two different analytical solutions proposed in the literature with the special aim to clarify their prominent features, the numerical advantages and the different physical implications of each of them. In particular, we will compare the temporal evolution of the obtained temperature in the case of spontaneously spreading, fully dynamic rupture on a fault of finite width and we will show how the solutions can be reconciled.I.N.G.V.Published3.1. Fisica dei terremotiope
Determination of the temperature field due to frictional heating on a sliding interface
No full textIn the recent years we assisted to an increasing number of studies devoted to the quantification of the effects of temperature developed as a consequence of frictional heat on a sliding interface. The temperature field generated on the fault surface is responsible of a large number of physical and chemical dissipative process, summarized in Bizzarri (2010a).
Among these we mention here the flash heating of micro–asperity contacts, basically consisting in a different behavior of fault friction at high fault slip velocities [e.g., Bizzarri, 2009a; Noda et al., 2009], the melting of rocks and gouge particles [Nielsen et al., 2008; Bizzarri, 2010b], the thermally–induced pressurization of fluids in saturated fault structures [Andrews, 2002; Bizzarri and Cocco, 2006; Rice, 2006].
A key issue of all these studies is the proper calculation of the temperature distribution on the fault surface and its temporal evolution.
In this study we compare two different analytical solutions proposed in the literature with the special aim to clarify their prominent features, the numerical advantages and the different physical implications of each of them. In particular, we will compare the temporal evolution of the obtained temperature in the case of spontaneously spreading, fully dynamic rupture on a fault of finite width and we will show how the solutions can be reconciled.I.N.G.V.Published3.1. Fisica dei terremotiope
Intracellular pH measurements made simple by fluorescent protein probes and the phasor approach to fluorescence lifetime imaging
No full textA versatile pH-dependent fluorescent protein was applied to intracellular pH measurements by means of the phasor approach to fluorescence lifetime imaging. By this fit-less method we obtain intracellular pH maps under resting or altered physiological conditions by single-photon confocal or two-photon microscopy. RI Bizzarri, Ranieri/H-1779-201
Determination of the temperature field due to frictional heating on a sliding interface
No full textIn the recent years we assisted to an increasing number of studies devoted to the quantification of the effects of temperature developed as a consequence of frictional heat on a sliding interface. The temperature field generated on the fault surface is responsible of a large number of physical and chemical dissipative process, summarized in Bizzarri (2010a).
Among these we mention here the flash heating of micro–asperity contacts, basically consisting in a different behavior of fault friction at high fault slip velocities [e.g., Bizzarri, 2009a; Noda et al., 2009], the melting of rocks and gouge particles [Nielsen et al., 2008; Bizzarri, 2010b], the thermally–induced pressurization of fluids in saturated fault structures [Andrews, 2002; Bizzarri and Cocco, 2006; Rice, 2006].
A key issue of all these studies is the proper calculation of the temperature distribution on the fault surface and its temporal evolution.
In this study we compare two different analytical solutions proposed in the literature with the special aim to clarify their prominent features, the numerical advantages and the different physical implications of each of them. In particular, we will compare the temporal evolution of the obtained temperature in the case of spontaneously spreading, fully dynamic rupture on a fault of finite width and we will show how the solutions can be reconciled.I.N.G.V.Published3.1. Fisica dei terremotiope
Determination of the temperature field due to frictional heating on a sliding interface
No full textIn the recent years we assisted to an increasing number of studies devoted to the quantification of the effects of temperature developed as a consequence of frictional heat on a sliding interface. The temperature field generated on the fault surface is responsible of a large number of physical and chemical dissipative process, summarized in Bizzarri (2010a).
Among these we mention here the flash heating of micro–asperity contacts, basically consisting in a different behavior of fault friction at high fault slip velocities [e.g., Bizzarri, 2009a; Noda et al., 2009], the melting of rocks and gouge particles [Nielsen et al., 2008; Bizzarri, 2010b], the thermally–induced pressurization of fluids in saturated fault structures [Andrews, 2002; Bizzarri and Cocco, 2006; Rice, 2006].
A key issue of all these studies is the proper calculation of the temperature distribution on the fault surface and its temporal evolution.
In this study we compare two different analytical solutions proposed in the literature with the special aim to clarify their prominent features, the numerical advantages and the different physical implications of each of them. In particular, we will compare the temporal evolution of the obtained temperature in the case of spontaneously spreading, fully dynamic rupture on a fault of finite width and we will show how the solutions can be reconciled.I.N.G.V.Published3.1. Fisica dei terremotiope
Introducción: Cultura y crisis ambiental en América Latina (numero monografico coordinado por Joaquín Barriendos, Gabriele Bizzarri, Stefano Tedeschi)
No full textAlvaro Bizzarri : migration, militance et cinéma
Full text linkEn 1963, un fonctionnaire de police est chargé de rédiger une première fiche de Bizzarri, ouvrier militant. A partir de 1970, quand Bizzarri devient cinéaste, son dossier auprès de la police politique prend de l’ampleur. Durant près de trente ans, Bizzarri cherche par le biais du cinéma à dénoncer les conditions, à ses yeux discriminatoires, dans lesquelles vivent ses compatriotes. Peu enclin à soutenir cette activité militante, le gouvernement helvétique ne financera jamais la production de ..
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