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A nonlinear Fokker-Planck equation modelling the approach to thermal equilibrium in a homogeneous plasma\ud

机译:非线性Fokker-Planck方程,模拟均质等离子体中的热平衡方法

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摘要

This work deals with the problem consisting in the equation (1) partial derivative f/partial derivative t = 1/x(2) partial derivative/partial derivative x [x(4)(partial derivative f/partial derivative x + f + f(2))], when x is an element of (0, infinity), t > 0, together with no-flux conditions at x = 0 and x = +infinity, i.e. (2) x(4)( partial derivative f/partial derivative x + f + f(2))=0 as x --> 0 or x --> +infinity. Such a problem arises as a kinetic approximation to describe the evolution of the radiation distribution f(x,t) in a homogeneous plasma when radiation interacts with matter via Compton scattering. We shall prove that there exist solutions of (1), (2) which develop singularities near x = 0 in a finite time, regardless of how small the initial number of photons N(0) = integral(0)(+infinity) x(2) f(x, 0)dx is. The nature of such singularities is then analyzed in detail. In particular, we show that the flux condition (2) is lost at x = 0 when the singularity unfolds. The corresponding blow-up pattern is shown to be asymptotically of a shock wave type. In rescaled variables, it consists in an imploding travelling wave solution of the Burgers equation near x = 0, that matches a suitable diffusive profile away from the shock. Finally, we also show that, on replacing (2) near x = 0 as determined by the manner of blow-up, such solutions can be continued for all times after the onset of the singularity.\ud
机译:这项工作处理的问题包括在等式(1)中偏导数f /偏导数t = 1 / x(2)偏导数/偏导数x [x(4)(偏导数f /偏导数x + f + f (2))],当x是(0,无穷大)的元素时,t> 0,以及x = 0和x = +无穷大的无通量条件,即(2)x(4)(偏导数f /偏导数x + f + f(2))= 0为x-> 0或x-> +无穷大。当辐射通过康普顿散射与物质相互作用时,这种问题以动力学近似的形式出现,描述了均匀等离子体中辐射分布f(x,t)的演变。我们将证明存在(1),(2)的解,它们在有限的时间内在x = 0附近产生奇点,而不管光子的初始数目N(0)=积分(0)(+无穷大)x (2)f(x,0)dx是然后详细分析这种奇异性的性质。特别地,我们表明,当奇点展开时,通量条件(2)在x = 0时丢失。相应的爆炸图显示为渐近的冲击波类型。在重新定标的变量中,它包括Burgers方程在x = 0附近的内爆行波解,它与远离冲击的合适扩散曲线匹配。最后,我们还表明,在替换由爆破方式确定的x = 0附近的(2)时,这样的解可以在奇异点出现后一直持续下去。

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