By Prof. Weston M. Stacey(auth.)
This revised and enlarged moment variation of the preferred textbook and reference includes accomplished remedies of either the proven foundations of magnetic fusion plasma physics and of the newly constructing components of energetic examine. It concludes with a glance forward to fusion strength reactors of the long run. The well-established issues of fusion plasma physics -- easy plasma phenomena, Coulomb scattering, drifts of charged debris in magnetic and electrical fields, plasma confinement by way of magnetic fields, kinetic and fluid collective plasma theories, plasma equilibria and flux floor geometry, plasma waves and instabilities, classical and neoclassical delivery, plasma-materials interactions, radiation, and so forth. -- are totally constructed from first ideas via to the computational types hired in smooth plasma physics.
the hot and rising subject matters of fusion plasma physics study -- fluctuation-driven plasma shipping and gyrokinetic/gyrofluid computational method, the physics of the divertor, impartial atom recycling and shipping, impurity ion delivery, the physics of the plasma part (diffusive and non-diffusive shipping, MARFEs, ELMs, the L-H transition, thermal-radiative instabilities, shear suppression of shipping, speed spin-up), and so on. -- are comprehensively built and on the topic of the experimental facts. Operational limits at the functionality of destiny fusion reactors are constructed from plasma physics and engineering constraints, and conceptual designs of destiny fusion strength reactors are mentioned.
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Extra info for Fusion Plasma Physics, Second Edition
Example text
2) where we identify W with the total kinetic energy. 1) also yields, for the z-component of motion, zR D 0 The solution of Eq. 3) k D const, so that Wk Á 12 m 2 k D const. Taken together 1 with Eq. 2), this result implies W? Á W Wk D const, so that ? 2W? =m/ 2 D const. In other words, the kinetic energy and speeds perpendicular to and parallel to the field are separately constants of the motion. The x- and y-components of Eq. 2) can be Fusion Plasma Physics. Weston M. Stacey © 2012 Wiley-VCH Verlag GmbH & Co.
4) ˝ xP where eB m is the gyrofrequency. 6) ˝ xR D ˝ 2 yP Now Eqs. 6) can be solved for the particle speeds zP D k xP D ? ˝t yP D ? ˝t C ˛/ where ˛ is a constant phase angle, and Eqs. 7) can be integrated to obtain xD ? ˝t C ˛/ C x0 ? 9) and gyromotion about the field line with angular frequencyq ˝ and gyroradius rL D ? 10) ˝ This gyromotion is oppositely directed for positive and negative charges, as shown in Fig. 1. Hz/ 2 1:5 107 B (protons) 2:7 1010 B (electrons) and p W? m/ 1:5 10 B p W? (electrons) 3:0 10 6 B when W?
The simple mirror is poloidally symmetric about the centerline. r; s/ D const defines the flux surfaces upon which the trapped particle guiding centers move, to first order. These flux surfaces are the surfaces of revolution about the centerline of the field lines shown in Fig. 1. Now we must examine the effects of drifts upon the particle motion. The curvature and grad-B drifts both produce net currents in the simple mirror. However, for the poloidally symmetric field, BÂ D @B=@Â D 0, and the B rB directed drifts and currents are in the poloidal direction and are poloidally symmetric.