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Dive into the research topics where Jenny-Ann Malmberg is active.

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Featured researches published by Jenny-Ann Malmberg.


Nuclear Fusion | 2001

Dust particles in controlled fusion devices: morphology, observations in the plasma and influence on the plasma performance

M. Rubel; Marco Cecconello; Jenny-Ann Malmberg; G. Sergienko; W. Biel; James Robert Drake; Anders Hedqvist; Alexander Huber; V. Philipps

The formation and release of particle agglomerates, i.e. debris and dusty objects, from plasma facing components and the impact of such materials on plasma operation in controlled fusion devices has been studied in the Extrap T2 reversed field pinch and the TEXTOR tokamak. Several plasma diagnostic techniques, camera observations and surface analysis methods were applied for in situ and ex situ investigation. The results are discussed in terms of processes that are decisive for dust transfer: localized power deposition connected with wall locked modes causing emission of carbon granules, brittle destruction of graphite and detachment of thick flaking co-deposited layers. The consequences for large next step devices are also addressed.


Nuclear Fusion | 2003

Overview of quasi-single helicity experiments in reversed field pinches

P. Martin; L. Marrelli; G. Spizzo; P. Franz; P. Piovesan; I. Predebon; T. Bolzonella; S. Cappello; A. Cravotta; D. F. Escande; L. Frassinetti; S. Ortolani; R. Paccagnella; D. Terranova; B.E. Chapman; D. Craig; Stewart C. Prager; J.S. Sarff; Per Brunsell; Jenny-Ann Malmberg; James Robert Drake; Yasuyuki Yagi; Haruhisa Koguchi; Y. Hirano; R. B. White; C.R. Sovinec; C. Xiao; Richard A. Nebel; D. D. Schnack

We report the results of an experimental and theoretical international project dedicated to the study of quasi-single helicity (QSH) reversed field pinch (RFP) plasmas. The project has involved several RFP devices and numerical codes. It appears that QSH spectra are a robust feature common to all the experiments. Our results expand and reinforce the evidence that the formation of self-organized states with one dominant helical mode (Ohmic SH state) is an approach complementary to that of active control of magnetic turbulence to improve confinement in a steady state RFP.


Physics of Plasmas | 2003

Resistive wall modes in the EXTRAP T2R reversed-field pinch

Per Brunsell; Jenny-Ann Malmberg; Dimitry Yadikin; Marco Cecconello

Resistive wall modes (RWM) in the reversed field pinch are studied and a detailed comparison of experimental growth rates and linear magnetohydrodynamic (MHD) theory is made. RWM growth rates are e ...


Physics of Plasmas | 2000

Locked modes in two reversed-field pinch devices of different size and shell system

Jenny-Ann Malmberg; Per Brunsell; Yasuyuki Yagi; Haruhisa Koguchi

The behavior of locked modes in two reversed-field pinch devices, the Toroidal Pinch Experiment (TPE-RX) [Y. Yagi et al., Plasma Phys. Control. Fusion 41, 2552 (1999)] and Extrap T2 [J. R. Drake et al., in Plasma Physics and Controlled Nuclear Fusion Research 1996, Montreal (International Atomic Energy Agency, Vienna, 1996), Vol. 2, p. 193] is analyzed and compared. The main characteristics of the locked mode are qualitatively similar. The toroidal distribution of the mode locking shows that field errors play a role in both devices. The probability of phase locking is found to increase with increasing magnetic fluctuation levels in both machines. Furthermore, the probability of phase locking increases with plasma current in TPE-RX despite the fact that the magnetic fluctuation levels decrease. A comparison with computations using a theoretical model estimating the critical mode amplitude for locking [R. Fitzpatrick et al., Phys. Plasmas 6, 3878 (1999)] shows a good correlation with experimental results in...


Physics of Plasmas | 2002

Resistive wall instabilities and tearing mode dynamics in the EXTRAP T2R thin shell reversed-field pinch

Jenny-Ann Malmberg; Per Brunsell

Observations of resistive wall instabilities and tearing mode dynamics in the EXTRAP T2R thin shell (τw=6 ms) reversed field pinch are described. A nonresonant mode (m=1,n=−10) with the same handedness as the internal field grows nearly exponentially with an average growth time of about 2.6 ms (less than 1/2 of the shell time) consistent with linear stability theory. The externally nonresonant unstable modes (m=1,n>0), predicted by linear stability theory, are observed to have only low amplitudes (in the normal low-Θ operation mode of the device). The radial field of the dominant internally resonant tearing modes (m=1,n=−15 to n=−12) remain low due to spontaneous fast mode rotation, corresponding to angular phase velocities up to 280 krad/s. Phase aligned mode structures are observed to rotate toroidally with an average angular velocity of 40 krad/s, in the opposite direction of the plasma current. Toward the end of the discharge, the radial field of the internally resonant modes grows as the modes slow d...


Plasma Physics and Controlled Fusion | 2002

Study of the confinement properties in a reversed-field pinch with mode rotation and gas fuelling

Marco Cecconello; Jenny-Ann Malmberg; P Nielsen; R Pasqualotto; James Robert Drake

An extensive investigation of the global confinement properties in different operating scenarios in the rebuilt EXTRAP T2R reversed-field pinch (RFP) experiment is reported here. In particular, the role of a fast gas puff valve system, used to control plasma density, on confinement is studied. Without gas puffing, the electron density decays below 0.5×1019 m−3. The poloidal beta varies between 5% and 15%, decreasing at large I/N. The energy confinement time ranges from 70 to 225 μs. With gas puffing, the density is sustained at ne≈1.5×1019 m−3. However, a general slight deterioration of the plasma performances is observed for the same values of I/N: the plasma becomes cooler and more radiative. The poloidal beta is comparable to that in the scenarios without puff but the energy confinement time drops ranging from 60 to 130 μs. The fluctuation level and the energy confinement time have been found to scale with the Lundquist number as S−0.05±0.07 and S0.5±0.1, respectively. Mode rotation is typical for all the discharges and rotation velocity is observed to increase with increasing electron diamagnetic velocity.


Physics of Plasmas | 2005

Observations of toroidicity-induced Alfvén eigenmodes in a reversed field pinch plasma

G. Regnoli; Henric Bergsåker; E. Tennfors; F. Zonca; E. Martines; G. Serianni; M. Spolaore; N. Vianello; Marco Cecconello; V. Antoni; R. Cavazzana; Jenny-Ann Malmberg

High frequency peaks in the spectra of magnetic field signals have been detected at the edge of Extrap-T2R [P. R. Brunsell, H. Bergsaker, M. Cecconello, J. R. Drake, R. M. Gravestijn, A. Hedqvist, and J.-A. Malmberg, Plasma Phys. Controlled Fusion, 43, 1457 (2001)]. The measured fluctuation is found to be mainly polarized along the toroidal direction, with high toroidal periodicity n and Alfvenic scaling (f∝B∕mini). Calculations for a reversed field pinch plasma predict the existence of an edge resonant, high frequency, high-n number toroidicity-induced Alfven eigenmode with the observed frequency scaling. In addition, gas puffing experiments show that edge density fluctuations are responsible for the rapid changes of mode frequency. Finally a coupling with the electron drift turbulence is proposed as drive mechanism for the eigenmode.


Japanese Journal of Applied Physics | 2002

Measurement of Vacuum Vessel Current and its Relation to Locked Mode in a Reversed-field Pinch Device, TPE-RX

Haruhisa Koguchi; Yasuyuki Yagi; Jenny-Ann Malmberg; Yoichi Hirano; Toshio Shimada; Hajime Sakakita; Shigeyuki Sekine

One of the hypotheses for the cause of the locked mode in reversed-field pinch (RFP) plasmas is examined using a large RFP machine, TPE-RX. A hypothetical model was proposed [Phys. Plasmas 6 (1999) 3824], which speculates that the halo current in the vacuum vessel might be the cause of the locked mode. We directly measured the toroidal distribution of the vessel current and correlated it with the position and the magnitude of the locked mode. The vessel current is found to flow into the contact point of the last closed flux surface where the locked mode exists. Magnitude of the vessel current is much smaller than the level expected to form the locked mode. From these observations, we conclude that this vessel current is a result of the local shift of the plasma column due to the locked mode, and may not be the cause of the locked mode.


Physica Scripta | 2001

Carbon particles emission, brittle destruction and co-deposit formation: experience from electron beam experiments and controlled fusion devices

J. Linke; M. Rubel; Jenny-Ann Malmberg; James Robert Drake; R. Duwe; H. Penkalla; M. R dig; E. Wessel


Physica Scripta | 2002

Self-Organisation and intermittent coherent oscillations in the EXTRAP-T2 reversed field pinch

Marco Cecconello; Jenny-Ann Malmberg; E. Sallander; James Robert Drake

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James Robert Drake

Royal Institute of Technology

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Per Brunsell

Royal Institute of Technology

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Haruhisa Koguchi

National Institute of Advanced Industrial Science and Technology

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Yasuyuki Yagi

National Institute of Advanced Industrial Science and Technology

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Dimitry Yadikin

Royal Institute of Technology

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M. Rubel

Royal Institute of Technology

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D. D. Schnack

Science Applications International Corporation

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Hajime Sakakita

National Institute of Advanced Industrial Science and Technology

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