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PROGRESS REPORT - ENEA - Fusione

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A1 Magnetic Confinement<br />

A Fusion Programme<br />

probes, due to the impact of μm-sized<br />

dust at a velocity of the order of ten km/s.<br />

This interpretation is supported directly<br />

by electron microscope analysis of the<br />

probe surface, which revealed the<br />

presence of 10 to 100–μm–sized craters,<br />

a typical footprint of the impact ionization<br />

processes (fig. A1.11). A number of<br />

spherically shaped, iron-rich μm-sized<br />

particles was also observed to be<br />

embedded in the probe surface. Neither<br />

craters nor embedded particles were<br />

detected on the surface of the “virgin”<br />

probe. The size, number and distribution<br />

of the observed craters are consistent<br />

with impact ionization processes<br />

Fig. A1.11 – Electron microscope analysis of the probe occurring at an average rate of a few<br />

surface<br />

hundred Hz, which corresponds to<br />

10 4 m -3 density of fast μm–sized dust<br />

particles accelerated at velocities of the order of 10 km/s by ion drag forces associated with plasma<br />

flows in the SOL of FTU.<br />

A1.4 Plasma Theory<br />

Mutual and positive feedbacks between theory and experiments have led to a clear identification of<br />

high-frequency MHD activity (high frequency with respect to that typical of MHD fluctuations) in FTU<br />

as evidence of nonlinear Alfvén mode excitations by a large magnetic island.<br />

Electron-fishbone mode excitations by LH additional power only are explained within a general<br />

theoretical framework, which fully accounts for the various experimental evidence of such modes<br />

and also provides a simple yet relevant model for interpreting the rich nonlinear dynamic behaviour,<br />

observed experimentally.<br />

The theory of propagation and absorption of rf waves in toroidal plasmas has been explored in both<br />

its more basic aspects as well as with detailed applications of practical relevance, such as the<br />

modelling of ICRH experiments in JET and the investigation of burning plasma dynamics issues by<br />

ICRH accelerated minority ion supra-thermal tails.<br />

The investigation of energetic ion dynamics in burning plasmas has been articulated along three<br />

main lines: i) identification of the relevant plasma parameters that make it possible to experimentally<br />

study burning plasma physics issues in sub-ignited regimes; ii) numerical simulation of energetic ion<br />

transport and nonlinear Alfvénic fluctuations in situations of experimental relevance in present-day<br />

experiments; iii) first-principle-based analysis of fundamental processes involved in the collective<br />

excitation of Alfvénic modes and in the fluctuation enhanced energetic ion transport. Item ii) has<br />

been explored with the interpretation of nonlinear Alfvén wave dynamics and energetic ion transport<br />

observed in JT-60U by means of hybrid MHD-gyrokinetic numerical simulations, carried out within<br />

an ongoing collaboration with the Japan Atomic Energy Agency. For item iii) an overview of the<br />

theory of Alfvén waves and energetic particle physics in burning plasmas has been given as a result<br />

of work done within the continuing collaboration with University of California at Irvine (UCI) USA.<br />

Within the same framework of UCI collaboration, recent theoretical work on plasma turbulence and<br />

turbulent transport, or more specifically, on nonlinear equilibria, stability and generation of zonal<br />

structures in toroidal plasmas has been summarised.<br />

Progress Report 2006<br />

16

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