Electrostatic and magnetostatic particle simulation models in three dimensions

by H. Okuda

Publisher: Dept. of Energy, Plasma Physics Laboratory, Publisher: for sale by the National Technical Information Service] in Princeton, N.J, [Springfield, Va

Written in English
Published: Pages: 22 Downloads: 476
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Subjects:

  • Particle accelerators,
  • Plasma confinement
  • Edition Notes

    Statementby H. Okuda, W. W. Lee, and C. Z. Cheng, Plasma Physica Laboratory, Princeton University
    SeriesPPPL ; 1461
    ContributionsLee, W. W., joint author, Cheng, C. Z., joint author, United States. Dept. of Energy, Princeton University. Plasma Physics Laboratory
    The Physical Object
    Pagination22 p. :
    Number of Pages22
    ID Numbers
    Open LibraryOL14882453M

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Directed Self-Assembly of Polarizable Ellipsoids in an External Electric FieldCited by: A particle of mass m moving with velocity V has kinetic energy equal to MV^2/2 (a scalar entity), and momentum equal to MV (a vector entity). These are two very different things. Suppose a particle of mass m is standing still, while another (identical) particle of the . A "massless particle" necessarily must travel with the speed of light (like a photon, the particle associated with light itself). But, if a particle has any mass, it may become arbitrarily close to and below the speed of light, but never equal to or greater. This book presents a comprehensive description of the physics of free-electron lasers starting from the fundamentals and proceeding through detailed derivations of the equations describing electron trajectories, and spontaneous and stimulated emission. as are detailed explanations of the nonlinear simulation of a variety of configurations.

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Electrostatic and magnetostatic particle simulation models in three dimensions by H. Okuda Download PDF EPUB FB2

Abstract. Several numerical plasma simulation models using particles are described which are appropriate for low frequency electrostatic and electromagnetic microinstabilities in a Cited by: 1. The collimated electron jets ejected from cylindrical plasma are produced in particle-in-cell simulation under the applied longitudinal magnetostatic field and radial electrostatic field, which is.

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Particle motion is the superposition of a large component due to the fluid drag toward the filter barrier and a random component due to brownian motion. We introduce the Peclet number Pe, which is the ratio between convective and diffusive displacement: – without a lattice, at each step the displacement is the sum of a constant vector U → (in flow direction) and r → with a random.

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Models and simulation. Finite. The voxel size is nm, at least a factor of 3 smaller than the voxel size obtained via FIB-nT. The particle dimensions are × × nm (X, Y, Z with respect to the image plane), giving it a slightly oblate profile. These dimensions mean that the particle is one of the smaller ones in the by: This is the first book on the fast multipole BEM, which brings together the classical theories in BEM formulations and the recent development of the fast multipole method.

Two- and three-dimensional potential, elastostatic, Stokes flow, and acoustic wave problems are covered, supplemented with exercise problems and computer source codes. Gauss's theorem with application, Electrostatic potential, boundary conditions, method of images, Laplace's and Poisson's equations, energy of an electrostatic system, conductor and dielectrics.

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