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Dive into the research topics where Yu. K. Kuznetsov is active.

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Featured researches published by Yu. K. Kuznetsov.


Nuclear Fusion | 2005

Plasma confinement using biased electrode in the TCABR tokamak

I. C. Nascimento; Yu. K. Kuznetsov; J. H. F. Severo; A. M. M. Fonseca; A. G. Elfimov; V. Bellintani; M. Machida; M.V.P. Heller; R. M. O. Galvão; E. Sanada; J. I. Elizondo

Experimental data obtained on the TCABR tokamak (R = 0.61?m, a = 0.18?m) with an electrically polarized electrode, placed at r = 0.16?m, is reported in this paper. The experiment was performed with plasma current of 90?kA (q = 3.1) and hydrogen gas injection adjusted for keeping the electron density at 1.0 ? 1019?m?3 without bias. Time evolution and radial profiles of plasma parameters with and without bias were measured. The comparison of the profiles shows an increase of the central line-averaged density, up to a maximum factor of 2.6, while H? hydrogen spectral line intensity decreases and the C?III impurity stays on the same level. The analysis of temporal behaviour and radial profiles of plasma parameters indicates that the confined plasma enters the H-mode regime. The data analysis shows a?maximum enhanced energy confinement factor of 1.95, decaying to 1.5 at the maximum of the density, in comparison with predicted Neo?Alcator scaling law values. Indications of transient increase of the density gradient near the plasma edge were obtained with measurements of density profiles. Calculations of turbulence and transport at the Scrape-Off-Layer, using measured floating potentials and ion saturation currents, show a strong decrease in the power spectra and transport. Bifurcation was not observed and the decrease in the saturation current occurs in 50??s.


Nuclear Fusion | 1992

Study of the magnetic configuration of an l=3 torsatron by the triode and the luminescent rod methods

G.G. Lesnyakov; E.D. Volkov; A.V. Georgievskij; V.M. Zalkind; Yu. K. Kuznetsov; F.I. Ozherel'ev; O.S. Pavlichenko; D.P. Pogozhev; K. Schworer; H. Hailer

The magnetic field configuration of the Uragan-3M l=3 torsatron, which has a p=4 multipole vertical magnetic field compensation system, was studied using two methods to map the contours of the magnetic flux surfaces. The first method, the so-called triode method with a constant voltage electron source, measures the current emitted by an open thermoelectron emitter and the portion drawn by a highly transparent grid located in a poloidal cross-section of the torus. The second method involves the use of a conducting luminescent rod which scans the torus cross-section and lights up when struck by electrons emitted by an electron gun. The information on the magnetic surface structure obtained by these two techniques is compared. The characteristics of the two methods are discussed, giving special attention to the triode method because it allows an objective criterion for the quality of the magnetic surface structure to be introduced. It is shown how advantageous both methods are for rapid adjustment and optimization of the magnetic configurations in a stellarator when perturbations are present and what improvements could be achieved on Uragan-3M. Also discussed are experiments on generating electron clouds in Uragan-3M during the ramp-up phase of the magnetic field pulse


Physics of Plasmas | 2008

Reduction of chaotic particle transport driven by drift waves in sheared flows

F. A. Marcus; Iberê L. Caldas; Z. O. Guimarães-Filho; P. J. Morrison; W. Horton; Yu. K. Kuznetsov; I. C. Nascimento

Investigations of chaotic particle transport by drift waves propagating in the edge plasma of tokamaks with poloidal zonal flow are described. For large aspect ratio tokamaks, the influence of radial electric field profiles on convective cells and transport barriers, created by the nonlinear interaction between the poloidal flow and resonant waves, is investigated. For equilibria with edge shear flow, particle transport is seen to be reduced when the electric field shear is reversed. The transport reduction is attributed to the robust invariant tori that occur in nontwist Hamiltonian systems. This mechanism is proposed as an explanation for the transport reduction in Tokamak Chauffage Alfven Bresilien [R. M. O. Galvao et al., Plasma Phys. Controlled Fusion 43, 1181 (2001)] for discharges with a biased electrode at the plasma edge.


Nuclear Fusion | 2007

Suppression and excitation of MHD activity with an electrically polarized electrode at the TCABR tokamak plasma edge

I. C. Nascimento; Yu. K. Kuznetsov; Z.O. Guimarães-Filho; I. El Chamaa-Neto; O. C. Usuriaga; A. M. M. Fonseca; R. M. O. Galvão; Iberê L. Caldas; J. H. F. Severo; I. Semenov; C. Ribeiro; M.V.P. Heller; V. Bellintani; J. I. Elizondo; E. Sanada

Two reproducible regimes of tokamak operation, with excitation or suppression of MHD activity can be obtained using a voltage-biased electrode inside the edge of the TCABR tokamak. The experiment was carried out adjusting the tokamak parameters to obtain two types of discharges: with strong or weak MHD activity, without biasing in both cases. The plasma current was adjusted to cover a range of safety factor from 2.9 up to 3.5, so that when biasing was applied the magnetic island (3,1) could interact with the edge barrier. The application of biasing in subsequent discharges of each type resulted in excitation or suppression of the MHD activity. The results show that the dominant modes are m = 2, n = 1 and m = 3, n = 1 for excitation and partial suppression, respectively. In both regimes a strong decrease in the radial electric field is detected with destruction of the transport barrier and of the improved confinement caused by different mechanisms. The measurements include temporal behaviour of edge transport, turbulence, poloidal electric and magnetic fields, edge density, radial electric fields and radial profile of Hα line intensity. The explanation of the excitation and suppression processes is discussed in the paper.


Nuclear Fusion | 1983

Determination of the plasma column shape in a tokamak from magnetic measurements

G.N. Deshko; T.G. Kilovataya; Yu. K. Kuznetsov; V.N. Pyatov; I.V. Yasin

On the basis of differential and integral methods of solving the boundary value problem and with the help of poloidal-magnetic-field or flux measurements by means of probes located outside the vacuum chamber, methods which are insensitive to measurement errors are developed for determining the position and shape of the boundary magnetic surface in a tokamak.


Nuclear Fusion | 2004

Runaway discharges in TCABR

Yu. K. Kuznetsov; R. M. O. Galvão; V. Bellintani; A A Ferreira; A. M. M. Fonseca; I. C. Nascimento; L. Ruchko; E. A. Saettone; V. S. Tsypin; O. C. Usuriaga

It is found in experiments carried out in Tokamak Chauffage Alfven Bresilien (TCABR) that two regimes of runaway discharges (RADs) with very different characteristics are possible. The RAD-I regime, which is similar to that observed in other tokamaks, can be obtained by a gradual transfer from a normal resistive to a RAD by decreasing the plasma density. This regime can be well understood using the Dreicer theory of runaway generation. The total toroidal current contains a substantial resistive component and the discharge retains some features of standard tokamak discharges. The second runaway regime, RAD-II, was recently discovered in the TCABR tokamak (Galvao R.M.O. et al 2001 Plasma Phys. Control. Fusion 43 1181). The RAD-II regime starts just from the beginning of the discharge, provided that certain initial conditions are fulfilled and, in this case, the runaway tail carries almost the full toroidal current. The background plasma is cold and detached from the limiter due to the recombination process. The primary Dreicer process is suppressed in the RAD-II and the secondary avalanche process dominates, even at the start-up phase, in the generation of the toroidal current. It is possible to trigger a transition from the RAD-I to the RAD-II regime using plasma cooling by gas puffing. The experimental results are shown to be in reasonable agreement with theoretical predictions based on the runaway avalanche process.


Physics of Plasmas | 2009

Bicoherence in electrostatic turbulence driven by high magnetohydrodynamic activity in Tokamak Chauffage Alfvén Brésilien

G. Z. dos Santos Lima; Z. O. Guimarães-Filho; A.M. Batista; I. L. Caldas; S.R. Lopes; I. C. Nascimento; Yu. K. Kuznetsov

During some discharges in Tokamak Chauffage Alfven Bresilien [R. M. O. Galvao et al., Plasma Phys. Controlled Fusion 43, 1181 (2001)] high magnetohydrodynamic activity may appear with a peaked frequency spectrum. Whenever this peak occurs, the ambient broadband electrostatic turbulence is remarkably modified, synchronizing into the dominant magnetic fluctuation frequency and presenting high bicoherence in the whole plasma edge with a maximum bicoherence inside the plasma. A phenomenological model is introduced to investigate this driven turbulence bicoherence, consisting of nonlinearly coupled phase-randomized drift modes with time-periodic external driving at the dominant magnetic fluctuation frequency. The bicoherence spectrum of this model can mimic features of the experimental results.


Physics of Plasmas | 2010

Recurrence quantification analysis of turbulent fluctuations in the plasma edge of Tokamak Chauffage Alfvén Brésilien tokamak

Z. O. Guimarães-Filho; I. L. Caldas; I. C. Nascimento; Yu. K. Kuznetsov; J. Kurths

Recurrences are close returns of a given state in a time series, and can be used to identify different dynamical regimes and other related phenomena, being particularly suited for analyzing experimental data. In this work, we use recurrence quantification analysis to investigate dynamical patterns in scalar data series obtained from measurements of floating potential and ion saturation current at the plasma edge of the Tokamak Chauffage Alfven Bresilien [R. M. O. Galvao et al., Plasma Phys. Controlled Fusion 43, 1181 (2001)]. We consider plasma discharges with and without the application of radial electric bias, and also with two different regimes of current ramp. Our results indicate that biasing improves confinement through destroying highly recurrent regions within the plasma column that enhance particle and heat transport.


Physics of Plasmas | 2008

Multifractality in plasma edge electrostatic turbulence

C Rodrigues Neto; Z. O. Guimarães-Filho; Iberê L. Caldas; I. C. Nascimento; Yu. K. Kuznetsov

Plasma edge turbulence in Tokamak Chauffage Alfven Bresilien (TCABR) [R. M. O. Galvao et al., Plasma Phys. Contr. Fusion 43, 1181 (2001)] is investigated for multifractal properties of the fluctuating floating electrostatic potential measured by Langmuir probes. The multifractality in this signal is characterized by the full multifractal spectra determined by applying the wavelet transform modulus maxima. In this work, the dependence of the multifractal spectrum with the radial position is presented. The multifractality degree inside the plasma increases with the radial position reaching a maximum near the plasma edge and becoming almost constant in the scrape-off layer. Comparisons between these results with those obtained for random test time series with the same Hurst exponents and data length statistically confirm the reported multifractal behavior. Moreover, the persistence of these signals, characterized by their Hurst exponent, present radial profile similar to the deterministic component estimated...


Nuclear Fusion | 1998

PLASMA BOUNDARY DETERMINATION IN ITER BY THE OPTIMIZED CURRENT FILAMENT METHOD

Yu. K. Kuznetsov; I. C. Nascimento; R. M. O. Galvão; I.V. Yasin

An accurate and simple technique for plasma boundary determination in a tokamak from external magnetic measurements is described. The method uses the filamentary current model of the plasma current profile, optimized to comply with the requirement of 1 cm accuracy in the determination of the plasma boundary in ITER. An error analysis is performed by numerical simulation of the ITER plasma configuration. The conclusion is that the method can provide this accuracy provided that the level of relative measurement errors can be kept below 1%.

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E. Sanada

University of São Paulo

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J. I. Elizondo

University of São Paulo

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L. Ruchko

University of São Paulo

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W.P. de Sá

University of São Paulo

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A. G. Elfimov

University of São Paulo

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