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Dive into the research topics where M. Ferrara is active.

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Featured researches published by M. Ferrara.


Nuclear Fusion | 2009

Experimental vertical stability studies for ITER performance and design guidance

D.A. Humphreys; T.A. Casper; N.W. Eidietis; M. Ferrara; D.A. Gates; Ian H. Hutchinson; G.L. Jackson; E. Kolemen; J.A. Leuer; J.B. Lister; L.L. LoDestro; W.H. Meyer; L.D. Pearlstein; A. Portone; F. Sartori; M.L. Walker; A.S. Welander; S.M. Wolfe

United States Department of Energy (DE-FC02-04ER54698, DEAC52- 07NA27344, and DE-FG02-04ER54235)


Nuclear Fusion | 2005

Overview of the Alcator C-Mod program

M. Greenwald; D. Andelin; N. Basse; S. Bernabei; P.T. Bonoli; B. Böse; C. Boswell; Ronald Bravenec; B. A. Carreras; I. Cziegler; E. Edlund; D. Ernst; C. Fasoli; M. Ferrara; C. Fiore; R. Granetz; O. Grulke; T. C. Hender; J. Hosea; D.H. Howell; A. Hubbard; J.W. Hughes; Ian H. Hutchinson; A. Ince-Cushman; James H. Irby; B. LaBombard; R. J. LaHaye; L. Lin; Y. Lin; B. Lipschultz

Research on the Alcator C-Mod tokamak has emphasized RF heating, self-generated flows, momentum transport, scrape-off layer (SOL) turbulence and transport and the physics of transport barrier transitions, stability and control. The machine operates with P-RF up to 6 MW corresponding to power densities on the antenna of 10 MW m(-2). Analysis of rotation profile evolution, produced in the absence of external drive, allows transport of angular momentum in the plasma core to be computed and compared between various operating regimes. Momentum is clearly seen diffusing and convecting from the plasma edge on time scales similar to the energy confinement time and much faster than neo-classical transport. SOL turbulence and transport have been studied with fast scanning electrostatic probes situated at several poloidal locations and with gas puff imaging. Strong poloidal asymmetries are found in profiles and fluctuations, confirming the essential ballooning character of the turbulence and transport. Plasma topology has a dominant effect on the magnitude and direction of both core rotation and SOL flows. The correlation of self-generated plasma flows and topology has led to a novel explanation for the dependence of the H-mode power threshold on the del B drift direction. Research into internal transport barriers has focused on control of the barrier strength and location. The foot of the barrier could be moved to larger minor radius by lowering q or B-T. The barriers, which are produced in C-Mod by off-axis RF heating, can be weakened by the application of on-axis power. Gyro-kinetic simulations suggest that the control mechanism is due to the temperature dependence of trapped electron modes which are destabilized by the large density gradients. A set of non-axisymmetric coils was installed allowing intrinsic error fields to be measured and compensated. These also enabled the determination of the mode locking threshold and, by comparison with data from other machines, provided the first direct measurement of size scaling for the threshold. The installation of a new inboard limiter resulted in the reduction of halo currents following disruptions. This effect can be understood in terms of the change in plasma contact with the altered geometry during vertical displacement of the plasma column. Unstable Alfven eigenmodes (AE) were observed in low-density, high-power ICRF heated plasmas. The damping rate of stable AEs was investigated with a pair of active MHD antennae.


Nuclear Fusion | 2007

Overview of the Alcator C-MOD Research Program

Stacey D. Scott; A. Bader; M. Bakhtiari; N. Basse; W. Beck; T. M. Biewer; S. Bernabei; P.T. Bonoli; B. Böse; Ronald Bravenec; I.O. Bespamyatnov; R. Childs; I. Cziegler; R.P. Doerner; E. Edlund; D. Ernst; A. Fasoli; M. Ferrara; C. Fiore; T. Fredian; A. Graf; T. Graves; R. Granetz; N.L. Greenough; M. Greenwald; M. Grimes; O. Grulke; D. Gwinn; R. W. Harvey; S. Harrison

Alcator C-MOD has compared plasma performance with plasma-facing components (PFCs) coated with boron to all-metal PFCs to assess projections of energy confinement from current experiments to next-generation burning tokamak plasmas. Low-Z coatings reduce metallic impurity influx and diminish radiative losses leading to higher H-mode pedestal pressure that improves global energy confinement through profile stiffness. RF sheath rectification along flux tubes that intersect the RF antenna is found to be a major cause of localized boron erosion and impurity generation. Initial lower hybrid current drive (LHCD) experiments (PLH < 900?kW) in preparation for future advanced-tokamak studies have demonstrated fully non-inductive current drive at Ip ~ 1.0?MA with good efficiency, Idrive = 0.4 PLH/neoR (MA, MW, 1020?m?3,m). The potential to mitigate disruptions in ITER through massive gas-jet impurity puffing has been extended to significantly higher plasma pressures and shorter disruption times. The fraction of total plasma energy radiated increases with the Z of the impurity gas, reaching 90% for krypton. A positive major-radius scaling of the error field threshold for locked modes (Bth/B ? R0.68?0.19) is inferred from its measured variation with BT that implies a favourable threshold value for ITER. A phase contrast imaging diagnostic has been used to study the structure of Alfv?n cascades and turbulent density fluctuations in plasmas with an internal transport barrier. Understanding the mechanisms responsible for regulating the H-mode pedestal height is also crucial for projecting performance in ITER. Modelling of H-mode edge fuelling indicates high self-screening to neutrals in the pedestal and scrape-off layer (SOL), and reproduces experimental density pedestal response to changes in neutral source, including a weak variation of pedestal height and constant width. Pressure gradients in the near SOL of Ohmic L-mode plasmas are observed to scale consistently as , and show a significant dependence on X-point topology. Fast camera images of intermittent turbulent structures at the plasma edge show they travel coherently through the SOL with a broad radial velocity distribution having a peak at about 1% of the ion sound speed, in qualitative agreement with theoretical models. Fast D? diagnostics during gas puff imaging show a complex behaviour of discrete ELMs, starting with an n ? 10 precursor oscillation followed by a rapid primary ejection as the pedestal crashes and then multiple, slower secondary ejections.


Nuclear Fusion | 2008

Plasma inductance and stability metrics on Alcator C-Mod

M. Ferrara; Ian H. Hutchinson; S.M. Wolfe

The growth rate of the vertical instability of elongated plasmas increases with the internal inductance. An upper limit to the value of the internal inductance is found, based on analytic approximations, and validated through the analysis of a large database of Alcator C-Mod plasmas. The extrapolation to ITER suggests that low-current high-q95 plasmas could exceed the original design value of li and thus be more difficult to stabilize. Metrics to characterize the vertical stability of tokamak plasmas are discussed and calculated for typical and ITER-like C-Mod plasmas. These figures contribute to the assessment of the ITER vertical stabilization loop and the establishment of what performance margin is required.


conference on decision and control | 2006

Alcasim simulation code for Alcator C-Mod

M. Ferrara; Ian H. Hutchinson; S.M. Wolfe; Joshua Stillerman; Thomas M. Fredian

A Matlab-Simulink simulation code Alcasim has been developed for Alcator C-Mod. The simulator includes models of the tokamak and plasma, the magnetic diagnostics and the power supplies. Alcasim runs the real-time control code of Alcator C-Mod and has been integrated with the standard software available to design the target waveforms and control algorithms. Extensive testing of the simulator has shown good agreement with experimental data. The short simulation time, which is around 3 minutes on a standard PC, makes Alcasim a close to real-time tool available to the physics operator to test the control programming in between C-Mod discharges. The Matlab-Simulink-IDL environment of Alcasim is also suitable to test new algorithms and architectures off-line and to develop advanced model-based control strategies


Fusion Science and Technology | 2009

State Reconstruction and Noise Reduction by Kalman Filter in the Vertical Position Control on Alcator C-Mod

M. Ferrara; Ian H. Hutchinson; S. M. Wolfe

Abstract The main sources of noise and pickups in Alcator C-Mod are identified, and their effects on the measurement and control of the vertical position are evaluated. Broadband noise may affect controllability of C-Mod plasmas at limit elongations and may become an issue with high-order controllers; therefore, two applications of Kalman filters are investigated. A Kalman filter is compared to a state observer based on the pseudoinverse of the measurement matrix and proves to be a better candidate for state reconstruction for vertical stabilization, provided adequate models of the system, the inputs, the process, and measurement noise and an adequate set of diagnostic measurements are available. A single-input single-output application of the filter for the vertical observer rejects high-frequency noise without destabilizing high-elongation plasmas.


Fusion Engineering and Design | 2006

Digital real-time plasma control system for Alcator C-Mod

J. Stillerman; M. Ferrara; T. Fredian; S.M. Wolfe


Assistant to Ian Hutchinson | 2009

Experimental vertical stability studies for ITER performance and design

Ian H. Hutchinson; S.M. Wolfe; M. Ferrara; D.A. Humphreys; T.A. Casper; N.W. Eidietis; D.A. Gates; G.L. Jackson; E. Kolemen; J.A. Leuer; J.B. Lister; L.L. LoDestro; W.H. Meyer; L.D. Pearlstein; A. Portone; F. Sartori; M.L. Walker; A.S. Welander


Archive | 2008

Axisymmetric Equilibrium and Stability Analysis in Alcator C-Mod, Including Effects of Current Profile, Measurement Noise and Power Supply Saturation

M. Ferrara


Bulletin of the American Physical Society | 2008

Current Saturation Avoidance with Real-Time Control using DPCS

M. Ferrara; Ian H. Hutchinson; S.M. Wolfe; J. Stillerman; T. Fredian

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Ian H. Hutchinson

Massachusetts Institute of Technology

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S.M. Wolfe

Massachusetts Institute of Technology

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T. Fredian

Massachusetts Institute of Technology

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J. Stillerman

Massachusetts Institute of Technology

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S. M. Wolfe

Massachusetts Institute of Technology

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D.A. Gates

Princeton Plasma Physics Laboratory

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E. Kolemen

Princeton Plasma Physics Laboratory

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