Modeling of CollisionsGauthier-Villars, 1998 - 222 من الصفحات |
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الصفحة 31
... electrons and ions is necessary . Between b and c , electrons can be treated as a fluid , ions still being kinetic . Between c and d , two - temperature hydrodynamics can be used . After d , one - temperature hydrodynamics is enough ...
... electrons and ions is necessary . Between b and c , electrons can be treated as a fluid , ions still being kinetic . Between c and d , two - temperature hydrodynamics can be used . After d , one - temperature hydrodynamics is enough ...
الصفحة 72
... electrons are light targets , and ions a are heavy ones . As we have seen ( section 3.1 ) , light targets disappear from perturbation equations . Light ions find themselves in front of heavy ions like electrons in front of ions [ 4-6,11 ...
... electrons are light targets , and ions a are heavy ones . As we have seen ( section 3.1 ) , light targets disappear from perturbation equations . Light ions find themselves in front of heavy ions like electrons in front of ions [ 4-6,11 ...
الصفحة 131
... ( electrons e and ions ) with reference frequencies ( 2-13 ) . B.1 wp » Vee The electron - electron collision frequency is never the largest collision frequency , but the proof is easy . According to appendix A , InЛee = ln kmaz kD 2Te 2 ...
... ( electrons e and ions ) with reference frequencies ( 2-13 ) . B.1 wp » Vee The electron - electron collision frequency is never the largest collision frequency , but the proof is easy . According to appendix A , InЛee = ln kmaz kD 2Te 2 ...
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appear approximation assumed atomic average Boltzmann Equation calculation chapter charge classical close collision frequencies collision terms collisional computed conservation consider correct Coulomb logarithms coupled defined density depend developed diffusion distribution function effect electrons energy equal equilibrium estimate existence expressions finally fluid flux formula frame given gives heat heavy hydrodynamic integrals interaction ion species ionic kinetic light limit linear mass Maxwellian mean mean velocity momentum multi-fluid neutral Note numerical obtained operator parameter particle particular perturbation perturbation equations Phys physics plasma pressure problem properties quantities quantum quantum mechanical reduced reference relations relative satisfies scalar single solution solved temperature tensor theory thermal transport coefficients transport equations vector αβ Μα