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Titlebook: An Introduction to the Linear Theories and Methods of Electrostatic Waves in Plasmas; W. D. Jones,H. J. Doucet,J. M. Buzzi Book 1985 Sprin

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期刊全称An Introduction to the Linear Theories and Methods of Electrostatic Waves in Plasmas
影响因子2023W. D. Jones,H. J. Doucet,J. M. Buzzi
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图书封面Titlebook: An Introduction to the Linear Theories and Methods of Electrostatic Waves in Plasmas;  W. D. Jones,H. J. Doucet,J. M. Buzzi Book 1985 Sprin
影响因子Modern plasma physics, encompassing wave-particle interactions and collec­ tive phenomena characteristic of the collision-free nature of hot plasmas, was founded in 1946 when 1. D. Landau published his analysis of linear (small­ amplitude) waves in such plasmas. It was not until some ten to twenty years later, however, with impetus from the then rapidly developing controlled­ fusion field, that sufficient attention was devoted, in both theoretical and experimental research, to elucidate the importance and ramifications of Landau‘s original work. Since then, with advances in laboratory, fusion, space, and astrophysical plasma research, we have witnessed important devel­ opments toward the understanding of a variety of linear as well as nonlinear plasma phenomena, including plasma turbulence. Today, plasma physics stands as a well-developed discipline containing a unified body of powerful theoretical and experimental techniques and including a wide range of appli­ cations. As such, it is now frequently introduced in university physics and engineering curricula at the senior and first-year-graduate levels. A necessary prerequisite for all of modern plasma studies is the under­ standin
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Tatjana Derr,Stefan Georg,Chris Heilerree space the resulting wave equation is a linear second-order partial-differential equation. Thus, the equations describing wave propagation in a complex medium such as a plasma can be complicated and difficult to solve directly. A technique that is widely used for solving such linear differential
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https://doi.org/10.1007/978-3-658-38282-7rgy except the energy alternately gained and lost as a result of their participation in the wave motion. In this chapter, we restrict our study to the behavior of electrostatic waves propagating parallel to the applied magnetic field in so-called warm plasmas, which are characterized by charged part
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https://doi.org/10.1007/978-3-658-34434-4ed any kind of wave damping or instability from our model so that both . and . were real quantities. We want to continue the study of the preceding chapter, except that we now want to include in our model collisions between charged particles and neutrals, and calculate what effects these collisions
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