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Plasma particles

Ultrafine powders can be prepared in high-temperature plasmas. Particles below 1 [Lm and larger particles with unusual surface structures are formed according to WaJdie [Trans. Inst. Chem. Eng., 48(3), T90 (1970)]. Energy costs are discussed. [Pg.1866]

In the previous section the interaction of the plasma particle flux with the surface of graphite was discussed. However, the fate of the implanted particles (most importantly deuterium and tritium) following their impact with the graphite surface is also an important issue, and is seen by some as the major impediment to graphite s use as a PFM [58], Quantification of the problem, and determination of possible mitigating steps, is complicated by experimental data which can vary by orders of magnitude [59-66] as reviewed by Wilson [67]. [Pg.420]

On the basis of the presented oscillator-wave model it is also possible to create heuristic models of the interaction of electromagnetic waves with plasma particles in the Earth s ionosphere and magnetosphere, heuristic models of the generation of powerful low-frequency waves in the space around the Earth when a cosmic electromagnetic background is present etc. High-efficient sub-millimeter emitter, built on this basis, could be suitable for radio-physical heating of plasma, e.g. in the experiments aimed the achievement of controlable thermonuclear reaction [ ] ... [Pg.119]

Dawson. J.M. Plasma Particle Accelerators," Sci. Amer., 54 (March 1989). Dehmelt, H. Experiments on the Structure of an Individual Elementary Particle, Science, 539 (February 2, 1990). [Pg.1218]

PLASMA (Particle). 1 An assembly of ions, electrons, neutral atoms and molecules in which the motion of the particles is dominated by electromagnetic interactions. This condition occurs when the macroscopic electrostatic shielding distance (Debye length) is small compared to the dimensions of the plasma. Because of the large electrostatic potentials... [Pg.1314]

Let us now consider the problem of bound states in plasmas. The interaction between the plasma particles is given by the Coulomb force. A characteristic feature of this interaction is its long range. Therefore, Coulomb systems show a collective behavior, so we can observe, for instance, the dynamical screening of the Coulomb potential and plasma oscillations. [Pg.228]

The question of surface chemical reactivity is critically dependent on the chemical nature and composition of the wall and the chemical nature and energies of the particles arriving at the wall. It will be necessary to develop experimental techniques to monitor the changing chemical composition of the first wall resulting from the flux of catalytic reactive plasma particles. Since the presence of active forms of hydrogen is inherent in all fusion devices, the potential for problems associated with surface chemical reactions of these species will always be present, only the form and magnitude of the problem will change. [Pg.76]

Fig. 10.1 Positive space charge layer at the interface between a plasma and (a) a dielectric, (b) a metallic, (c) an electrolytic wall with floating potential w- Due to the negative surface charge mainly neutral, positive and only high energetic negative plasma particles reach the wall (je- flow of electrons, j <+ flow of cations, ji< flow of neutralized particles, jA- flow of anions). The potential difference between the zero poten-... Fig. 10.1 Positive space charge layer at the interface between a plasma and (a) a dielectric, (b) a metallic, (c) an electrolytic wall with floating potential <t>w- Due to the negative surface charge mainly neutral, positive and only high energetic negative plasma particles reach the wall (je- flow of electrons, j <+ flow of cations, ji< flow of neutralized particles, jA- flow of anions). The potential difference between the zero poten-...
Fig. 2.6. Top section of computational domain for TEXTOR model, showing also the cross-section of the toroidal ALT-II limiter 45 degrees underneath the outer mid-plane. Bottom computed Balmer-alpha emission profile (photons/s/cm3, logarithmic colour scale) in the TEXTOR edge plasma, as used for interpretation of visible spectroscopy [26] and determination of plasma particle confinement... Fig. 2.6. Top section of computational domain for TEXTOR model, showing also the cross-section of the toroidal ALT-II limiter 45 degrees underneath the outer mid-plane. Bottom computed Balmer-alpha emission profile (photons/s/cm3, logarithmic colour scale) in the TEXTOR edge plasma, as used for interpretation of visible spectroscopy [26] and determination of plasma particle confinement...
Divertor erosion/co-deposition estimates in ITER are based on the RE-DEP/WBC code package [98-100]. Power fluxes as well as plasma particle fluxes (i.e., D-T ions and atoms, and impurities such as helium and carbon)... [Pg.305]

The basic reference model for the case of collisionless plasma background with regard to the absorption of plasma particles by the grain, the OML theory, has been initiated by the paper of Bernstein and Rabinovitz [14], As mentioned in this work, the asymptotical behavior of the screened potential for collisionless case is inversely proportional to the square distance the authors also formulate here the question about the role of the bound ionic states in the grain... [Pg.292]


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See also in sourсe #XX -- [ Pg.154 ]




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