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  • 1
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A series of experiments has been carried out to determine the relative screening of the low recycling gaseous impurities, nitrogen and methane, in Alcator C-Mod tokamak [Phys. Plasmas 1, 1511 (1994)] discharges. The impurity density in the core plasma is directly proportional to the rate of impurity injection. Screening was found to vary weakly with plasma density but to be markedly dependent on the poloidal position of injection. Detachment of the plasma results in significantly less screening both in Ohmic and in high confinement (H-mode) discharges, particularly when the gas is injected into the divertor or at the inner vessel wall. Evidence of impurity transport from the scrape-off layer into the divertor using bolometry and visible spectroscopy is presented and modeling of the transport using a two-dimensional Monte Carlo code is described. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 2 (1995), S. 707-715 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In the absence of drifts, the Bohm–Chodura criterion gives that the fluid velocity parallel to the magnetic field reaches the ion acoustic speed at the entrance to the magnetic presheath. The changes to this criterion are derived for the situation where poloidal E×B drifts are present. (It was shown earlier that diamagnetic drifts do not influence this criterion.) Here E×B drifts can cause the parallel fluid velocity at the magnetic presheath entrance to become supersonic, subsonic, or reversed (negative). © 1995 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 2 (1995), S. 702-706 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The ion flow velocity entering the Debye sheath is constrained to satisfy the Bohm criterion: velocity must be equal to or greater than sonic. The ion flow velocity entering the magnetic presheath (which arises upstream of the Debye sheath when a magnetic field, oblique to the solid surface is present) is constrained to satisfy the Chodura criterion: velocity-parallel to B must be equal to or greater than sonic. The Bohm criterion, in its marginal form where v=cs, is associated with a "gentle entry'' into the sheath with Δne=Δni, while v(approximately-greater-than)cs corresponds to ||Δne||(approximately-greater-than)||Δni||. The magnetic presheath, in contrast with the Debye sheath, is a region of quasineutrality, and thus only Δne=Δni is permitted. This might appear to prohibit supersonic flow parallel to B at the entrance to the magnetic presheath, which the analysis of Chodura and Riemann has found to be permitted, in fact. This apparent contradiction is resolved by analyzing the magnetic presheath region to bring out more explicitly the role played by inertia in the E×B direction, thus confirming that such supersonic flow is permitted. © 1995 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 1 (1989), S. 1133-1140 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Four models of collisionless one-dimensional plasma flow to a boundary are compared with regard to their predictions of particle and heat fluxes to the boundary for a given plasma density and temperature far from the boundary. The models include two kinetic treatments, that of Emmert et al. [Phys. Fluids 23, 803 (1980)], and that of Bissell and Johnson [Phys. Fluids 30, 779 (1987)], an isothermal fluid model, Self and Ewald [Phys. Fluids 9, 2486 (1966) and Stangeby, [Phys. Fluids 27, 2699 (1984)], and an adiabatic fluid model, Zawaideh, Najmabadi, and Conn [Phys. Fluids 29, 463 (1986)]. The fluid models do not explicitly include collisions; however, the adiabatic closure condition employed, namely, neglect of ion heat conduction, implies a degree of ion self-collisionality. It is found that the particle and heat fluxes to the boundary differ very little among the four models—spanning a range of about ±10%. It is therefore concluded that, with regard to modeling of such important practical quantities as outfluxes, a simple and convenient formulation, such as the isothermal fluid model, is adequate. Substantial differences among the models are found for certain other predicted quantities, namely, the spatial variation of ion temperature along the flow and the magnitude of the electric field near the boundary.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 31 (1988), S. 2726-2727 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In a recently published probe theory Hutchinson argues that the cross-field viscosity coefficient n⊥≈ρD⊥, where ρ is the mass density and D⊥ is the diffusion coefficient. This argument is questioned.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 9 (2002), S. 3489-3507 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Simple, analytic models are developed to estimate the plasma particle fluxes to the main chamber walls of a divertor tokamak in terms of assumed values of the cross-field transport coefficients, D⊥, v⊥, and of the wall–gap size. The wall–gap size is the cross-field width of the gap between the last closed flux surface, LCFS, defined by magnetic (divertor) separatrix and the wall of the main chamber, the "wall-limiter." The neutrals recycling from the wall may be ionized at, or inboard of, the LCFS—which is a key feature of the so-called "simple SOL" and which is referred to here as the pure transport case. On the other hand, the neutrals may be ionized within the scrape-off layer, SOL, in the main chamber, with the ions returning to the wall—referred to here as the SOL ionization case. SOL ionization gives rise to a radial flux amplification effect, in the sense that the plasma flux to the walls is larger than for the "simple SOL"—all else held equal, including the separatrix density, wall–gap, and the transport coefficients. The amplification factor is found to be only modest, however, up to ∼2x. Primarily, plasma–wall contact is therefore just simply a function of cross-field plasma transport, which is strongly anomalous in the SOL, probably due to turbulence, and possibly intermittent, large-event activity in the outer regions. The experimental database for D⊥SOL, v⊥SOL is weak, particularly for the far SOL, a situation calling for increased experimental and theoretical effort. © 2002 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 30 (1987), S. 3262-3267 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Insertion of a probe into the plasma induces a high speed flow of the hydrogenic plasma to the probe which, by friction, accelerates the impurity ions to velocities approaching the hydrogenic ion acoustic speed, i.e., higher than the impurity ion thermal speed. A simple analytic theory based on this effect provides a relation between impurity fluxes to the probe Γimp and the undisturbed impurity ion density nimp, with the hydrogenic temperature and density as input parameters. Probe size also influences the collection process and large probes are found to attract a higher flux density than small probes in the same plasma. The quantity actually measured, cimp, the impurity atom surface density (m−2) net-deposited on the probe, is related to Γimp and thus to nimp by taking into account the partial removal of deposited material caused by sputtering and the redeposition process.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 28 (1985), S. 644-651 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: When large probes are used to measure plasma properties in tokamak scrape-off layers, the presence of the probe influences the plasma being measured. A theory is presented for probe interpretation which makes it possible to infer undisturbed values of Te, Ti, ne, etc. The first requirement in such an analysis is for analytic models of the scrape-off layer, which can then be modified to allow for the presence of the probe. The present work gives such a model for the collisionless scrape-off layer, and criteria are stated governing its applicability. Such models may be of use for other applications, e.g., predictions of power loading to limiter surfaces, the magnitude of wall sputtering, etc.
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  • 9
    Electronic Resource
    Electronic Resource
    [s.l.] : Nature Publishing Group
    Nature 233 (1971), S. 472-473 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] The present communication suggests the possibility that such a double discharge could form the basis of an isotope separator, if the outer, irradiating discharge were run in a pure isotope and the hyperfine components of the resonance line are separate.,We show in Fig. 3 the hyperfine components of ...
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  • 10
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