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Перегляд Bопросы атомной науки и техники, 2008 за темою "Magnetic confinement"

Репозиторій DSpace/Manakin

Перегляд Bопросы атомной науки и техники, 2008 за темою "Magnetic confinement"

Сортувати за: Порядок: Результатів:

  • An l=2 torsatron with centered planar magnetic axis 
    Kotenko, V.G. (Вопросы атомной науки и техники, 2008)
    The paper is concerned with properties of magnetic surface configurations that have the planar magnetic axis coincident with the circular geometrical axis of the torus. The calculations were performed for the model of an ...
  • Appearance of neoclassical effects in plasma behavior in torsatron Uragan-3М 
    Pashnev, V.K.; Sorokovoy, Ed.L. (Вопросы атомной науки и техники, 2008)
    At present paper the existence of longitudinal current in plasma and time dependence of plasma density in experiments on torsatron U-3M are explained from the point of neoclassical theory. The time evolution of longitudinal ...
  • Effect of the resonance phenomena on high energetic particle losses in closed magnetic trap with the rotational transform of the magnetic field 
    Moskvitina, Yu.K.; Shishkin, A.A. (Вопросы атомной науки и техники, 2008)
    The mechanism of controlled resonant particle transport in the closed magnetic traps is studied. The resonance condition of the particle-magnetic field interaction is presented. The dependence of the resonance radial ...
  • Energy confinement in the torsatron Uragan-3M during the RF-heating mode 
    Pashnev, V.K.; Burchenko, P.Ya.; Lozin, A.V.; Kotsubanov, V.D.; Kulaga, A.Ye.; Krasnyj, V.V.; Mironov, Yu.K.; Nikol’skii, I.K.; Petrushenya, A.A.; Romanov, V.S.; Sitnikov, D.A.; Sorokovoy, Ed.L.; Tsybenko, S.A.; Zamanov, N.V. (Вопросы атомной науки и техники, 2008)
    Energy confinement time of plasma in torsatron U-3M was measured both during quasi-stationary stady of RF-discharge and after RF-power cut-off. Power absorbed by plasma in the confinement region was estimated. A mechanism ...
  • Influence of an external low frequency helical perturbation on ballooning modes 
    Pankratov, I.M.; Omelchenko, A.Ya. (Вопросы атомной науки и техники, 2008)
    Equations for investigation of the influence of external helical magnetic perturbations on the ballooning modes are derived in one-fluid MHD with the plasma response and rotation being taken into account.
  • Microwave diagnostic system of the Uragan-2М torsatron 
    Sitnikov, D.A.; Berezhnyj, V.L.; Larin, Y.V.; Maznichenko, S.M.; Ocheretenko, V.L.; Pinos, I.B.; Prokopenko, A.V.; Skibenko, A.I.; Tarasov, M.I. (Вопросы атомной науки и техники, 2008)
    The construction of microwave sections together with results of loss calculation in the microwave lines for different frequencies are presented. The construction of microwave lead-ins is also described. The whole system ...
  • Multislit electromagnetic trap “Jupiter F” 
    Lavrent’ev, O.A.; Maslov, V.A.; Krutko, N.A.; Oboznyj, V.P. (Вопросы атомной науки и техники, 2008)
    The construction of multislit electromagnetic trap “Jupiter F” with application of ferromagnetic materials to strengthening of a magnetic field, the results of calculations, and the results of experimental investigations ...
  • Role of radial electric field in LH transition triggered by counter-NBI at low plasma Density in the TUMAN-3M tokamak 
    Tukachinsky, A.S.; Askinazi, L.G.; Chernyshev, F.V.; Golant, V.E.; Irzak, M.A.; Kornev, V.A.; Krikunov, S.V.; Krupnik, L.I.; Lebedev, S.V.; Melnik, A.D.; Razumenko, D.V.; Rozhdestvensky, V.V.; Rushkevic, A.A.; Smirnov, A.I.; Vild’junas, M.I.; Zhubr, N.A. (Вопросы атомной науки и техники, 2008)
    Threshold power needed to attain H-mode in a tokamak is a critical parameter for designing of future devices and in particular fusion reactor ITER [1]. According to commonly accepted scaling [2] the threshold power Pthr ...
  • The interaction between broadband electromagnetic oscillations and plasma 
    Tarasov, I.K. (Вопросы атомной науки и техники, 2008)
    The interaction between plasma and HF oscillations in a broad frequency range is studied. To introduce the HF power into plasma an active antenna array was used. This allowed varying the phase velocity of the wave disturbed ...

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