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Titlebook: Introduction to Nonlinear Fluid-Plasma Waves; Bhimsen K. Shivamoggi Book 1988 Kluwer Academic Publishers, Dordrecht 1988 Soliton.electroma

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書目名稱Introduction to Nonlinear Fluid-Plasma Waves
編輯Bhimsen K. Shivamoggi
視頻videohttp://file.papertrans.cn/474/473966/473966.mp4
叢書名稱Mechanics of Fluids and Transport Processes
圖書封面Titlebook: Introduction to Nonlinear Fluid-Plasma Waves;  Bhimsen K. Shivamoggi Book 1988 Kluwer Academic Publishers, Dordrecht 1988 Soliton.electroma
描述A variety of nonlinear effects occur in a plasma. First, there are the wave- steepening effects which can occur in any fluid in which the propagation speed depends upon the wave-amplitude. In a dispersive medium this can lead to classes of nonlinear waves which may have stationary solutions like solitons and shocks. Because the plasma also acts like an inherently nonlinear dielectric resonant interactions among waves lead to exchange of energy among them. Further, an electromagnetic wave interacting with a plasma may parametrically excite other waves in the plasma. A large-amplitude Langmuir wave undergoes a modulational instability which arises through local depressions in plasma density and the corresponding increases in the energy density of the wave electric field. Whereas a field collapse occurs in two and three dimensions, in a one-dimensional case, spatially localized stationary field structures called Langmuir solitons can result. Many other plasma waves like upper-hybrid waves, lower-hybrid waves etc. can also undergo a modulational instability and produce localized field structures. A new type of nonlinear effect comes into play when an electromagnetic wave propagating th
出版日期Book 1988
關(guān)鍵詞Soliton; electromagnetic wave; electron; model; oscillation; scattering; stability; turbulence
版次1
doihttps://doi.org/10.1007/978-94-009-2772-8
isbn_softcover978-94-010-7746-0
isbn_ebook978-94-009-2772-8Series ISSN 0921-3805
issn_series 0921-3805
copyrightKluwer Academic Publishers, Dordrecht 1988
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Nonlinear Ion-Acoustic Waves,hermodynamic equilibrium at a constant temperature . in these wave motions with a number density given by the Boltzmann distribution.where . is the electrostatic potential associated with the wavemotions, and . is the number density of electrons (or ions) in the unperturbed state. For low frequency
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Parametric Excitations of Plasma Waves, ways — either due to wave-wave interactions or due to temporal variations in the electromagnetic fields in the presence of a large-amplitude pump wave. We will consider in the following examples of both types of excitations.
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Nonlinear Waves in an Inhomogeneous Plasma,way in an inhomogeneous plasma. For instance, the amplitude, width, and propagation velocity of an ion-acoustic solitary wave will change as the latter moves in an inhomogeneous plasma (Nishikawa and Kaw [194], John and Saxena [195], Rao and Varma [196], Shivamoggi [197, 198], Kuehl [199, 200], Chan
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d in quickly locating useful information. The first edition of the reference will focus on high-impact solutions from the most recent decade; later editions will widen the scope of the work...Nearly 500 entries will be organized alphabetically by problem, with subentries allowing for distinct soluti
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Bhimsen K. Shivamoggid in quickly locating useful information. The first edition of the reference will focus on high-impact solutions from the most recent decade; later editions will widen the scope of the work...Nearly 500 entries will be organized alphabetically by problem, with subentries allowing for distinct soluti
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