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Chapter 2 Single particle motions21 Uniform magnetic field In this case, the equation of motion for a particle is(2-1) Takingto be the direction of, we have(2-2a)(2-2b)(2-2c)Differentiating (2-2a) and
Chapter 6 The Allocation of Depletable and Renewable Resources: An OverviewContents:71 Introduction72 A Resource Taxonomy73 Efficient IntertemporalAllocation74 Market Allocation75 Summary71 Introducti
Chapter 8Recyclable Resources: Minerals, Paper, Glass, Etc81 IntroductionQuestions to be resolved:What is an efficient amount of recyclingWill the market automatically generate this amount in the abse
Chapter 7 Depletable, Nonrecyclable Energy Resources: Oil, Gas, Coal, and Uranium71 IntroductionMain contents:This chapter will examine some of the major issues associated with the allocation of energ
Chapter 5 Applications of integralsAreas between curvesThe Riemann sumThereforeSolutionSolutionWe find that the points of intersection are(0, 0) and (1, 1)SoSolutionBy solving the system of equationso
811 Basic equationsChapter 8Sheath theory81 The collisionless sheathWe use the assumptions: (1) Maxwellian electrons at temperature(2) cold ions, and (3)at the plasma-sheathinterface at x= define the
Chapter 5 Distribution function of electrons in electric field51 Method for solving kinetic equationLet us consider in the case where a homogeneous electric field is the source of disequilibrium The e
Chapter 6 Plasma fluid equations 61 Distribution function moments equations611 Derivation of moments equationsLet us find the general form of the moments equations To this end we make use of the kinet
91 Representation of wavesChapter 9Waves in plasma Considering a plan wave, we can represent the density as follows(9-1)whereis a constant defining the amplitude of the wave,is the frequency of the wa
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