D. Frigione
ENEA
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Featured researches published by D. Frigione.
Plasma Physics and Controlled Fusion | 2002
X. Litaudon; F. Crisanti; B. Alper; Y. Baranov; E. Barbato; V. Basiuk; A. Bécoulet; M. Becoulet; C. Castaldo; C. D. Challis; G. D. Conway; R. Dux; L.-G. Eriksson; B. Esposito; C. Fourment; D. Frigione; X. Garbet; C. Giroud; N. C. Hawkes; P. Hennequin; G. Huysmans; F. Imbeaux; E. Joffrin; P. Lomas; Ph. Lotte; P. Maget; M. Mantsinen; J. Mailloux; F. Milani; D. Moreau
Quasi-steady operation has been achieved at JET in the high-confinement regime with internal transport barriers (ITBs). The ITB has been maintained up to 11 s. This duration, much larger than the energy confinement time, is already approaching a current resistive time. The high-performance phase is limited only by plant constraints. The radial profiles of the thermal electron and ion pressures have steep gradients typically at mid-plasma radius. A large fraction of non-inductive current (above 80%) is sustained throughout the high-performance phase with a poloidal beta exceeding unity. The safety factor profile plays an important role in sustaining the ITB characteristics. In this regime where the self-generated bootstrap current (up to 1.0 MA) represents 50% of the total current, the resistive evolution of the non-monotonic q-profile is slowed down by using off-axis lower-hybrid current drive.
Nuclear Fusion | 1996
D. Frigione; L. Pieroni; V. Zanza; G. Apruzzese; F. Alladio; M.L. Apicella; R. Bartiromo; M. Borra; G. Bracco; G. Buceti; P. Buratti; C. Centioli; M. Ciotti; V. Cocilovo; I. Condrea; F. Crisanti; R. De Angelis; B. Esposito; A. Frattolillo; G. Gatti; E. Giovannozzi; G. Granucci; M. Grolli; A. Imparato; H. Kroegler; M. Leigheb; L. Lovisetto; G. Maddaluno; G. Mazzitelli; P. Micozzi
Plasma behaviour in the high density regime has been investigated on the Frascati Tokamak Upgrade (FTU). The items particularly addressed are density limit, MARFE characteristics and fuelling efficiency. With gas puffing, a maximum line average density of 3.2*1020 m-3 has been obtained in the ohmic regime at q=5.1, corresponding to 1.7 times the Greenwald limit; while with pellet injection, a value of 3.7*1020 m-3 has been reached at q=3.5. The density limit appears to be connected with the impurity content and edge parameters, so the best results are obtained with very clean plasmas and peaked electron density profiles. The MARFE phenomenon always appears beyond a critical density that depends on the total input power and the effective charge: emissivities in the range of 2 to 12 MW/m3 have been measured in this highly radiating region. The fuelling efficiency, starting from a value of about 50% at low density, progressively deteriorates, falling to 10% near the density limit: this behaviour is interpreted as being due to a decrease of the scrape-off layer transparency to incoming neutrals
Journal of Nuclear Materials | 2003
B. Pégourié; E Tsitrone; R. Dejarnac; J. Bucalossi; G. Martin; J. Gunn; D. Frigione; D. Reiter; Ph. Ghendrih; C. Clement
Abstract A fueling system by supersonic pulsed gas injection has been installed on the high field side of Tore Supra. First results are encouraging, demonstrating a fueling efficiency four times higher than that of conventional gas puff. One-dimensional modeling shows that the increase of efficiency is linked to the short injection time and to the prompt cooling of the plasma edge consecutive to the massive injection of matter. Improvements of the system could lead to the formation of a high-β blob which could experience a drift down the magnetic field, analogously to pellet injection, thus further increasing the fueling efficiency of the method.
Plasma Physics and Controlled Fusion | 1997
P. Buratti; F Alladio; P Micozzi; O. Tudisco; L. Acitelli; B. Angelini; M L Apicella; G Apruzzese; E. Barbato; A. Bertocchi; G Bracco; A. Bruschi; G Buceti; A Cardinali; C Centioli; R Cesario; S. Ciattaglia; M. Ciotti; S Cirant; V Cocilovo; F. Crisanti; R. De Angelis; F. De Marco; B. Esposito; D. Frigione; L Gabellieri; G Gatti; E Giovannozzi; C. Gourlan; G. Granucci
The MHD activity of plasma configurations with reversed magnetic shear has been investigated on the FTU tokamak. In the presence of pairs of surfaces with the same rational value q = m/n of the safety factor, double-tearing modes are excited which give rise in most cases to bursts of sawtooth-like profile rearrangements. More stable regimes have also been found, in which the activity is dominated by rotating saturated modes. In a particular case with and a discharge without any detectable MHD activity during the current flat-top has been obtained. In high-temperature regimes ( at ), an irregular activity has been detected near the plasma centre which could be due to the excitation of resistive interchange modes.
Plasma Physics and Controlled Fusion | 1999
S Cirant; A. Airoldi; L. Bertalot; G Bracco; A. Bruschi; P. Buratti; G. Cenacchi; R. Coelho; F. Crisanti; B. Esposito; L Gabellieri; F. Gandini; G. Granucci; Enzo Lazzaro; H. Krögler; S Nowak; D Pacella; L Panaccione; G. Ramponi; A. Simonetto; C. Sozzi; O. Tudisco; M. Zerbini; F Alladio; B. Angelini; M L Apicella; G Apruzzese; E. Barbato; A. Bertocchi; M. Borra
Magnetohydrodynamic (MHD) activity and energy transport at rational-q surfaces is analysed on the basis of experimental results on current density profile control obtained with localized electron cyclotron resonance heating (ECRH) on FTU tokamak. The MHD response, in particular 2/1 and 1/1 modes, to ECRH is in agreement with expectations from a theoretical model including resistive wall braking and toroidal mode coupling. It is also shown that the magnetic shear atrqD1 could controlmD 1 mode saturation and magnetic reconnection. Heating results with ECRH at steady state indicate that transport enhancement is the dominant effect on confinement at theqD 2 surface, and suggest that conduction and convection inside the asymmetricmD 1 island should both be taken into account for a proper description of the thermal response to localized ECRH.
Nuclear Fusion | 2016
A. Murari; E. Peluso; M. Gelfusa; L. Garzotti; D. Frigione; M. Lungaroni; F. Pisano; P. Gaudio; Jet Contributors
Determination of causal-effect relationships can be a difficult task even in the analysis of time series. This is particularly true in the case of complex, nonlinear systems affected by significant ...
Nuclear Fusion | 2015
M. Lennholm; P. Beaumont; I. S. Carvalho; I. T. Chapman; R. Felton; D. Frigione; L. Garzotti; A. Goodyear; J. P. Graves; D. Grist; S. Jachmich; P. T. Lang; E. Lerche; E. de la Luna; R. Mooney; James R. Morris; M. F. F. Nave; F. Rimini; G. Sips; E. R. Solano; M. Tsalas; Jet-Efda Contributors
This paper describes the first development and implementation of a closed loop edge localized mode (ELM) frequency controller using gas injection as the actuator. The controller has been extensively used in recent experiments on JET and it has proved to work well at ELM frequencies in the 15–40xa0Hz range. The controller responds effectively to a variety of disturbances, generally recovering the requested ELM frequency within approximately 500xa0ms. Controlling the ELM frequency has become of prime importance in the new JET configuration with all metal walls, where insufficient ELM frequency is associated with excessive tungsten influx. The controller has allowed successful operation near the minimum acceptable ELM frequency where the best plasma confinement can be achieved. Use of the ELM frequency controller in conjunction with pellet injection has enabled investigations of ELM triggering by pellets while maintaining the desired ELM frequency even when pellets fail to trigger ELMs.
Nuclear Fusion | 1996
V. Zanza; S.E. Segre; L. Gabellieri; F. Alladio; M.L. Apicella; G. Apruzzese; R. Bartiromo; M. Borra; G. Bracco; G. Buceti; P. Buratti; C. Centioli; M. Ciotti; V. Cocilovo; I. Condrea; F. Crisanti; R. De Angelis; B. Esposito; A. Frattolillo; D. Frigione; E. Giovannozzi; G. Granucci; M. Grolli; A. Imparato; H. Kroegler; M. Leigheb; L. Lovisetto; G. Maddaluno; G. Mazzitelli; P. Micozzi
Three methods of density modulation have been used in FTU discharges (gas puffing, pellet injection and current rampup). The analysis of particle balance confirms that the neoclassical theory is not adequate and the experimental results obtained by the three methods are used to verify the validity of an empirical expression for the radial particle flux. Such an expression is relevant for the design of future experiments and constitutes a constraint for any satisfactory theory.
Plasma Physics and Controlled Fusion | 2012
Torbjörn Hellsten; Thomas Johnson; D. Van Eester; E. Lerche; Y. Lin; M.-L. Mayoral; J. Ongena; G. Calabrò; K. Crombé; D. Frigione; C. Giroud; M. Lennholm; P. Mantica; M. F. F. Nave; V. Naulin; C. Sozzi; W. Studholme; T. Tala; T. W. Versloot
The rotation of L-mode plasmas in the JET tokamak heated by waves in the ion cyclotron range of frequencies (ICRF) damped on electrons, is reported. The plasma in the core is found to rotate in the counter-current direction with a high shear and in the outer part of the plasma with an almost constant angular rotation. The core rotation is stronger in magnitude than observed for scenarios with dominating ion cyclotron absorption. Two scenarios are considered: the inverted mode conversion scenarios and heating at the second harmonic He-3 cyclotron resonance in H plasmas. In the latter case, electron absorption of the fast magnetosonic wave by transit time magnetic pumping and electron Landau damping (TTMP/ELD) is the dominating absorption mechanism. Inverted mode conversion is done in (He-3)-H plasmas where the mode converted waves are essentially absorbed by electron Landau damping. Similar rotation profiles are seen when heating at the second harmonic cyclotron frequency of He-3 and with mode conversion at high concentrations of He-3. The magnitude of the counter-rotation is found to decrease with an increasing plasma current. The correlation of the rotation with the electron temperature is better than with coupled power, indicating that for these types of discharges the dominating mechanism for the rotation is related to indirect effects of electron heat transport, rather than to direct effects of ICRF heating. There is no conclusive evidence that mode conversion in itself affects rotation for these discharges.
Plasma Physics and Controlled Fusion | 2011
E. Lerche; D. Van Eester; J. Ongena; M.-L. Mayoral; Martin Laxåback; F. Rimini; A. Argouarch; P. Beaumont; T. Blackman; V. Bobkov; D. Brennan; A. M. Brett; G. Calabrò; Marco Cecconello; I. Coffey; L Colas; A. Coyne; Kristel Crombé; A. Czarnecka; R. Dumont; F. Durodié; R. Felton; D. Frigione; M. Gatu Johnson; C. Giroud; G. Gorini; M. Graham; C. Hellesen; Torbjörn Hellsten; S. Huygen
In the past years, one of the focal points of the JET experimental programme was on ion-cyclotron resonance heating (ICRH) studies in view of the design and exploitation of the ICRH system being developed for ITER. In this brief review, some of the main achievements obtained in JET in this field during the last 5 years will be summarized. The results reported here include important aspects of a more engineering nature, such as (i) the appropriate design of the RF feeding circuits for optimal load resilient operation and (ii) the test of a compact high-power density antenna array, as well as RF physics oriented studies aiming at refining the numerical models used for predicting the performance of the ICRH system in ITER. The latter include (i) experiments designed for improving the modelling of the antenna coupling resistance under various plasma conditions and (ii) the assessment of the heating performance of ICRH scenarios to be used in the non-active operation phase of ITER.