... 2 , EX1 = 0, EX1 = 1, i = 1, 2, ..., cov (Xi , Xj ) = > 0 i = j. , ( lim P{Xnn) < n 2(1 - ) ln n + x} = (x/ ). ... 2 F (x) = 1 - e-x , x > 0. . ... 2). nlim P{Xnn) < x + ln n} = exp(x)(1 - exp(- exp(-x))), Tn = (n) ( nX1 + ln n Kn = Xnn) - ln n . ... 1 Xn = Xn-1 + n , r r 2- , { n }- , {0, 1/r, 2/r, ..., (r - 1)/r}, n X , n-1 , Xn U (0, 1). exp( 1 r-1 r n lim P{(X (n) n - 1)n < x} = x) , , x) , , x 0, x > 0, x 0, x < 0. n lim P{nX1 (n) < x} = 1 - exp(- 0 r -1 r Tn = (n) - 1)n Hn = nX1 . ...

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Introduction to PLASMA ASTROPHYSICS (Selected 10 lectures) Boris V. Somov Astronomical Institute and Faculty of Physics Moscow State University Pushino-na-Oke, 2008 Contents Ab out These Lectures 1 Particles and Fields: Exact Self-Consistent Description 1.1 Liouville's theorem . . . . . . . . . . . . . . . . . . . 1.1.1 Continuity in phase space . . . . . . . . . 1.1.2 The character of particle interactions 1.1.3 The Lorentz force, gravity . . . . . . . . . 1.1.4 Collisional friction . . . . . . . . . . . .

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