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  • 1
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Materials science forum Vol. 182-184 (Feb. 1995), p. 467-470 
    ISSN: 1662-9752
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Materials science forum Vol. 195 (Nov. 1995), p. 209-214 
    ISSN: 1662-9752
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 4 (1992), S. 1708-1723 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The stability of a magnetized plasma is investigated in which a sheared electron flow channel is present. The flow's peak velocity and shear scale length are denoted by V and L, respectively. If the velocity channel is perpendicular to the confining magnetic field and L≤ ρi (ρi is the ion Larmor radius) an electrostatic instability develops whose frequency is on the order of the lower hybrid frequency. For V/(ΩeL) (approximately-greater-than) 0.02 (Ωe denotes the electron cyclotron frequency), the peak growth rate is on the order of the lower hybrid frequency when k(parallel) = 0 (in here, k(parallel) is the wave number along the magnetic field). For V/(ΩeL) (approximately-greater-than) 0.1 and k(parallel) = 0, the spectrum peaks when kyL ∼ 1, where ky is the wave number in the direction of the flow velocity. For this mode it is shown that (i) a net cross-field current is not required for the onset of instability and (ii) the growth rate is not reduced by a velocity profile with no net flow (spatially averaged). Hence we conclude that velocity shear is the only source of free energy. Further, it is shown that density gradients do not stabilize this mode. It follows that the mode presented in this work cannot be identified with the well-known modified two-stream instability. If the velocity channel is parallel to the confining magnetic field and the plasma is weakly magnetized, an instability driven by velocity shear is shown to exist, provided that V/(ωpeL) (approximately-greater-than) 0.32, where ωpe is the electron plasma frequency. It is shown that a net plasma current is not required in order for this instability to be excited.
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  • 4
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 2 (1990), S. 2007-2023 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An analytic and numerical study is made of the effects caused by coherent density fluctuations, localized near the ion–ion hybrid resonance, on the propagation and absorption of fast Alfvén waves. The system is represented by a Budden equation that incorporates static fluctuations in the ion density profiles. The unperturbed system contains a resonance at x=0 and a cutoff at x=d; the Alfvén wave number at resonance is kA. Two cases are considered: fluctuations in the ion concentration ratio η and bulk density fluctuations. When the incident wave directly approaches the resonance, the fluctuation in the concentration ratio δη/η0 is less than 20%, and kAd〈1, a "renormalized'' Budden potential yields analytic expressions in good agreement with numerical results. In this regime, the reflection coefficient exhibits a new contribution arising from the modifications of the resonance layer. For direct approach, kAd〉1, and concentration fluctuations 2%〈δη/η0〈5%, enhanced reflection leads to decreased absorption. For these parameters, the net absorption is reduced by more than 10% for noise wave numbers larger than 10 kA. However, the efficiency of the resonant absorption process remains unaffected. For kAd〉2 and fluctuations δη/η0〉5%, a regime of multiple resonances is encountered in which substantial absorption results. For indirect approach, a similar process takes place: The reflection coefficient is reduced from its unperturbed ∼1 value to ∼0. For bulk fluctuations, backscattering is the dominant physical process.
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  • 5
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 1 (1989), S. 1805-1810 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: It is shown that second-order (ρ/L) corrections in the expression for the equilibrium distribution function are required to obtain a self-adjoint system of equations for ion cyclotron range of frequencies (ICRF) wave propagation in a nonuniform plasma (ρ denotes the ion-Larmor radius and L the gradient scale length). Self-adjointness results in energy conservation in the absence of absorption mechanisms, as expected. A Lagrangian density is obtained, which yields both the wave operator and its adjoint, and directly results in the conservation law of the truncated system.
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  • 6
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 5 (1993), S. 3163-3181 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A study is presented of the nonlinear evolution of a magnetized plasma in which a localized electron cross-field flow is present. The peak velocity of the flow is denoted by V0; LE represents the flow's shear scale length; and the regime ρe〈LE〈ρi is considered, where ρi and ρe denote the ion and electron Larmor radii, respectively. It is shown that if the shear frequency ωs=V0/LE is larger than the lower-hybrid frequency, ωLH, then the system dynamics is dominated by the onset of the electron–ion-hybrid (EIH) mode which leads to the formation of coherent (vortexlike) structures in the electrostatic potential of the ensuing lower-hybrid waves. The wavelength of these structures is on the order of LE, and correlates well with that predicted by the linear theory of the EIH mode. Since the characteristic wavelength is longer than ρe, the corresponding phase velocity is low enough that there results significant direct resonant ion acceleration perpendicular to the confining magnetic field. When ωs(approximately-greater-than)3ωLH, the system exhibits significant anomalous viscosity (typically an order of magnitude larger than that due to Coulomb collisions), which increases as the shear frequency is increased. As ωs is reduced below ωLH, shear effects are no longer dominant and a smooth transition takes place in which the system dynamics is governed by the short wavelength (on the order of ρe) lower-hybrid drift instability.
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  • 7
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 3 (1991), S. 2960-2966 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A numerical study is made of the effects caused by incoherent fluctuations in the minority density concentration on the absorption of fast Alfvén waves at the ion–ion hybrid resonance. This work extends to the incoherent regime of a previous study by Romero and Morales [Phys. Fluids B 2, 2007 (1990)], which surveyed in detail the effects of single-mode (coherent) fluctuations. The system is represented by a Budden equation that properly describes the resonance and cutoff structure arising from spatial variations of the equilibrium magnetic field. For wave incidence such that the cutoff is encountered before the resonance layer, the absorption coefficient increases monotonically as the fluctuation amplitude is increased. A specific case is presented in which the absorption changes from ∼0% to ∼70% for minority density fluctuations δn/n0∼60% that correspond to electron density variations of less than 5%. For wave incidence such that the resonance is encountered before the cutoff, the reflection coefficient increases for minority density fluctuations below 5% of the ambient value. For larger density fluctuations, the reflected energy saturates at ∼20% of the incident wave energy.
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  • 8
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 2 (1990), S. 3054-3058 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The inverse linear mode conversion between an electrostatic ion Bernstein wave and an electromagnetic fast Alfvén wave in tokamak plasmas is investigated using a self-adjoint system of equations of fourth order that includes cyclotron and Landau damping processes. Over a broad range of cases investigated, the reciprocity of the mode conversion coefficients between the ion Bernstein and fast waves is observed to hold, within numerical accuracy, even in the presence of strong cyclotron absorption. It is also found that strong bulk ion heating occurs at twice the cyclotron frequency for direct launching of an ion Bernstein wave into a plasma that contains no ionic species that are resonant at the fundamental cyclotron frequency.
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  • 9
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Food Chemistry 50 (1994), S. 389-392 
    ISSN: 0308-8146
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Agriculture, Forestry, Horticulture, Fishery, Domestic Science, Nutrition , Process Engineering, Biotechnology, Nutrition Technology
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  • 10
    Publication Date: 1992-12-14
    Print ISSN: 0031-9007
    Electronic ISSN: 1079-7114
    Topics: Physics
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