Alternating Dimension Plasma Transport in Three Dimensions
Alternating Dimension Plasma Transport in Three Dimensions
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In our eReader you can find the full English version of the book. Read Alternating Dimension Plasma Transport in Three Dimensions Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Alternating Dimension Plasma Transport in Three Dimensions
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4) first with J, then with B, and then average, to obtain = -^| + (4. 6) d * dt = -|l + P, ' f 1^2V 14 = (4. 7) = ip' (£±0-2 ~ f 2 a l^ It remains to evaluate the periods f, and f_. Taking the jump of (4. 3) across either E, or £», = [Va] || - V* [|£] + [Vf] .
Note that only the projection of [Va] is zero for a surface potential a. First take a = a. And the indicated jump across Z~ where [a. ]_= 1 [cf. (2. 8)]. This implies that [Va, ]- = and [3a /at], = 0, hence [f]y = c, (t) . Similarly, ...for a = a~, [g], = -c-(t). The remaining period of f or g can then be eliminated between (4. 6) and (4. 7) giving dip. Dip. 2 dl. Ip! 2 I!
(4 - 8) dt 1 = ' diT + d^ " c i= " p^ + p^ - Ci These are the two averaged flux conservation equations. They reduce to the conventional equations in the case of an ignorable coordinate (two dimensions, axial symmetry, helical symmetry), These equations could be used, in principle, to advance \p . In time, since the right side is known in terms of a given, instantaneous equilibrium state, Vp = J*b.
What to read after Alternating Dimension Plasma Transport in Three Dimensions?
You can find similar books in the "Read Also" column, or choose other free books by Harold Grad to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
4) first with J, then with B, and then average, to obtain
Note that only the projection of [Va] is zero for a surface potential a. First take a = a. And the indicated jump across Z~ where [a. ]_= 1 [cf. (2. 8)]. This implies that [Va, ]- = and [3a /at], = 0, hence [f]y = c, (t) . Similarly,
(4 - 8) dt 1 = ' diT
What to read after Alternating Dimension Plasma Transport in Three Dimensions?
You can find similar books in the "Read Also" column, or choose other free books by Harold Grad to read onlineMoreLess
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