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2 edition of effects of ion-ion collision on a[n] ion-acoustic plasma pulse found in the catalog.

effects of ion-ion collision on a[n] ion-acoustic plasma pulse

M. S. Espedal

effects of ion-ion collision on a[n] ion-acoustic plasma pulse

by M. S. Espedal

  • 95 Want to read
  • 36 Currently reading

Published in Bergen .
Written in English

    Subjects:
  • Ion acoustic waves.

  • Edition Notes

    Bibliography: leaf 19.

    Statementby Magne S. Espedal.
    SeriesUniversity of Bergen. Dept. of Applied Mathematics. Report no. 25
    Classifications
    LC ClassificationsQA801 .B4 no. 25
    The Physical Object
    Pagination20 [4] l.
    Number of Pages20
    ID Numbers
    Open LibraryOL4668749M
    LC Control Number77559395

      It is perhaps surprising that a process which was one of the first to be studied on an atomic scale, and a process which first received attention over seven decades ago, continues to be the object of diverse and intense research efforts. Such is the case with the (seemingly) conceptually simple and familiar mechanism of electron impact ionization of atoms, molecules, and ions. Abstract The process of collision of ion-acoustic solitary waves in a collisionless plasma with cold ions and Boltzmann electrons is studied using numerical simulations. It is shown that solitary waves with sufficiently large amplitudes do not preserve their identity after the collision. Their amplitudes decrease, and the shapes change.

    Ion-acoustic waves in a plasma with negative ions B. Song, N. D’ Angelo, and R. L. Merlin0 Department of Physics and Astronomy, The University of Iowa, Iowa City, Iowa (Received 14 May ; accepted 8 October ) Propagation and damping of ion-acoustic waves have been investigated in File Size: KB. the effective collision frequency n in the presence of current-driven ion-acoustic waves (CDIAW) was given as: n ¼ w pe e 0dE2 2nk BT e ð1Þ where w pe =(nq e 2/m e 0) 1/2 is the electron plasma frequency, n is the electron number density, T e is the electron temperature, and dE 2 is the observed wave power of the fluctuations. From n both.

    Learn more about the A/C and Pulse monitor application specs in-depth from Ion Physics Corp. For propagation in the perpendicular direction, maximum growth rates can be substantially larger than those of the zero magnetic field ion acoustic instability. For propagation outside a few degrees from the perpendicular the dispersion characteristics are essentially those of the ion acoustic by:


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Effects of ion-ion collision on a[n] ion-acoustic plasma pulse by M. S. Espedal Download PDF EPUB FB2

Collisional effects on ion-acoustic waves in a nonequilibrium plasma: Authors: Plasma Physics: Origin: STI: NASA/STI Keywords: Collisional Plasmas, Electron Scattering, Ion Acoustic Waves, Ionic Collisions, Landau Damping, Nonequilibrium Plasmas, Kinetic Equations, Mean Free Path, Particle Collisions, Phase Velocity, Plasma Interactions.

We have considered the effect of electron-ion collision on the structure of the solitary wave in a relativistic unmagnetized plasma. In the present analysis we have considered ions to be cold, the electrons hot.

The equation obtained for ion velocity is not the usual KdV type but a perturbed version of it, where the perturbing term is proportional to the electron-ion collision by: 1.

The ion-acoustic and Buneman instabilities are studied in a current carrying plasma by taking into account the collisional effects and q-nonextensive distribution the kinetic theory and Bhatnagar–Gross–Krook collision model, a generalized dielectric permittivity function in the presence of moving electrons and electron and ion–neutral collision frequency is by: 4.

Two-dimensional simulations with the BZOHAR [B. Cohen, B. Lasinski, A. Langdon, and E. Williams, Phys. Plasmas 4, ()] hybrid code (kinetic particle ions and Boltzmann fluid electrons) have been used to investigate the saturation of stimulated Brillouin backscatter (SBBS) instability, including the effects of ion-ion collisions and by:   This paper examines analytically the transition domain between collisionless and collision dominated flows in the environment of a plasma sheath.

The onset of collisions also brings into focus the concurrent effects due to ionization, which are retained in the : Pung Nien Hu, Sigi Ziering. After each collision, we store the value of the scattering angle Θ for each particle. We assume that whenever P sin2 Θ ‚ 1 the particle has undergone one ion-ion Coulomb collision.

Here the summation is over successive collisions for a given particle. Momentum exchange during a collision We treat Coulomb collisions between ions as a small. Dust–ion-acoustic wave propagation in an inhomogeneous plasma is studied for the case of density-dependent ion–dust collisions.

It is shown that, because of the interplay between the inhomogeneity and collisions, the relative amplitude of the wave first decreases and then increases with distance when the wave propagates down the density by: 5. For plasma with strongly developed ion-acoustic turbulence, an explicit expression for the ion collision integral was derived in the Bychenkov-Silin-Uryupin model [1].

View Show abstract. Measure the group velocity of the ion acoustic waves for a relative hot plasma and a relatively cold plasma, and test simpli ed perturbation the-ory results, that is, the dispersion relationship for ion acoustic waves, and from a direct measurement of kT e using the Langmuir probe, compare the-ory (calculating the phase velocity given the elec-File Size: KB.

For a magnetic-field-free plasma which slightly departs from equilibrium, we use Eq.(6) and let the distribution function be fα= fα0+fα1, where the letter α in the subscript of f denotes particle species (α=i, e; i for ion and e for electron), fα0 corresponds to the one-dimensional power-law q-equilibrium distribution (5), and fα1 is the corresponding perturbation about the distribution.

The effect of ion-ion collision on the dynamics of nonlinear ion acoustic wave in an unmagnetized pair-ion plasma has been investigated. The two-fluid model has been used to describe the dynamics of both positive and negative ions with equal masses.

It is well known that in the dynamics of the weakly nonlinear wave, the viscosity mediates wave dissipation in presence of weak nonlinearity Cited by: 4. Creating and studying ion acoustic waves in ultracold neutral plasmasa) T. Killian,1,b) P. McQuillen,2 T. O’Neil,2 and J. Castro1 1Department of Physics and Astronomy and Rice Quantum Institute, Rice University, Houston, TexasUSA 2Department of Physics, University of California at San Diego, La Jolla, CaliforniaUSA (Received 7 December ; accepted 4 January   I assume you are talking about ion-acoustic waves, which propagate in plasma.

These are simply oscillations of ions and electrons through a plasma of positively charged ions, which gives the waves the property to interact with each other due to the particles having electromagnetic charge. The effect of ion-ion collision on the dynamics of nonlinear ion acoustic wave in an unmagnetized pair-ion plasma has been investigated.

The two-fluid model has been used to describe the dynamics. The generation of ion-acoustic solitary waves is investigated in a nonuniform multicomponent collisional plasma sheath containing cold ions and Boltzmann electrons to probe the formation and physics of modulation of nonlinear ion-acoustic waves.

The new model for the plasma is adapted to include the effects of ion production-loss and momentum loss terms due to ion-neutral Author: Nora Nassiri-Mofakham. Collisions between electrons and ions 3 3. Electron-ion collision operator We start with the e ect on electrons of collisions with ions.

We perform an expansion in p m e=m i˝1. We rst consider the lowest order in p m e=m i˝1, and later we keep higher order terms. Electron-ion collision File Size: KB. The various aspects of the propagation of ion-acoustic waves have been intensively studied in non-uniform medium [] that are governed by modified KdV (mKdV) equation.

In the present work, we have derived a modified KdV equation describing the ion-acoustic solitary wave in presence of weak ion-neutral collision frequency.

A one-dimensional kinetic code is used to study the effect of ion-neutral (charge exchange and elastic scattering) and ion-ion collisions on plasma flow in the downstream region of an electron-cyclotron-resonance plasma etching system.

Ions are assumed to leave the source region at the Bohm velocity. Argon, nitrogen, and CF 4 plasmas are simulated, assuming that the dominant ion species are Ar Cited by: Some of the earliest civilizations regarded the universe as organized around four principles, the four "elements" earth.

water, air, and fire. Fire, which was the source of light and as such possessed an immaterial quality related to the spiritual world. was clearly the most impressive of theseBrand: Springer US. In plasma physics, an ion acoustic wave is one type of longitudinal oscillation of the ions and electrons in a plasma, much like acoustic waves traveling in neutral gas.

However, because the waves propagate through positively charged ions, ion acoustic waves can interact with their electromagnetic fields, as well as simple plasmas, ion acoustic waves are frequently referred to as. A magnetized plasma sheath where the ion collision frequency depends on ion flow velocity To cite this article: S Farhad Masoudi J.

Phys. D: Appl. Phys. 40 View the article online for updates and enhancements. Related content Collisional effects in magnetized plasma sheath with two species of positive ions M M Hatami, B Shokri and A R. We report experimental evidence of ion–ion acoustic instability in laser-produced astrophysically relevant plasma.

Irradiation of a copper foil with a short (2 ps) intense (10 17 W cm −2) laser pulse generates dense hot plasma, whose expansion into the rarefied preplasma generates the electrostatic collisionless : J. L. Jiao, S. K. He, H. B. Zhuo, B. Qiao, M. Y. Yu, M. Y. Yu, B. Zhang, Z. G. Deng, F. Lu, K.

N. Zh.The properties of nonlinear IA waves are significantly modified by the effects of nonplanar geometry, ion kinematic viscosity, and the degree of nonextensivity. The important findings of our results in astrophysical plasmas like stellar polytropes, hadronic matter, quark-gluon plasma, dark-matter halos, and so on are pinpointed in this : M.

Ferdousi.