Wave Propagation Across Ion Cyclotron Resonance Harmonic Layers
Wave Propagation Across Ion Cyclotron Resonance Harmonic Layers
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In our eReader you can find the full English version of the book. Read Wave Propagation Across Ion Cyclotron Resonance Harmonic Layers 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 Wave Propagation Across Ion Cyclotron Resonance Harmonic Layers
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To quickly assess the difficulty of the text, read a short excerpt:
We find the ion current to be the sum of (18) and (22). We readily observe that our boundary layer -35- expansion is consistent provided that 8 = e„, , (81) Xp/Xg = (Zp/Zg)''(nj, /ng)(mp/mg) = 2(Zg/Zp) (n^/ng) = 0(8).
We add the electron current obtained from the charge neutrality, drop terms of order m /m. , and eliminate E, to obtain e 1 - {1 + d^ + (1 + H + d^)[dA(s)d - B(s)]}E^ = 0, (82) where 2 2 \i = (e _ - nji )/ (e^, ^ ~ °|| ^ ' \ = (e__ - 4 )(%+ - 4 )/(e„ - 4 ).
d = d/ds.
s = -2£8n Ixo.../c. ^ c ^^^^ =^s"l, o/^^x-4>' B(s) =^^.
e -n XX II According to (81) the density ratio n^/n„=0(8) and this might seem to be an uninteresting parameter range. However, the numerical calculations given in Sec. VI show that a maximum in the wave energy absorption occurs with a rather small addition of minority species on the order of 1% of the electron number density. Such a small minority fraction is consistent with our ordering. We note that if the ordering (81) is not satisfied, within the layer E must get much smaller in magnitude in order to keep the first term in the right-hand side of the first equation in (22) balanced.
What to read after Wave Propagation Across Ion Cyclotron Resonance Harmonic Layers?
You can find similar books in the "Read Also" column, or choose other free books by Kaya Imre to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
We find the ion current to be the sum of (18) and (22). We readily observe that our boundary layer -35- expansion is consistent provided that 8 = e„, , (81) Xp/Xg = (Zp/Zg)''(nj, /ng)(mp/mg) = 2(Zg/Zp) (n^/ng) = 0(8).
We add the electron current obtained from the charge neutrality, drop terms of order m /m. , and eliminate E, to obtain e 1 - {1 + d^ + (1 + H + d^)[dA(s)d - B(s)]}E^ = 0, (82) where 2 2 \i = (e _ - nji )/ (e^, ^ ~ °|| ^ ' \ = (e__ - 4 )(%+ - 4 )/(e„ - 4 ).
d = d/ds.
s = -2£8n Ixo.../c. ^ c ^^^^ =^s"l, o/^^x-4>' B(s) =^^.
e -n XX II According to (81) the density ratio n^/n„=0(8) and this might seem to be an uninteresting parameter range. However, the numerical calculations given in Sec. VI show that a maximum in the wave energy absorption occurs with a rather small addition of minority species on the order of 1% of the electron number density. Such a small minority fraction is consistent with our ordering. We note that if the ordering (81) is not satisfied, within the layer E must get much smaller in magnitude in order to keep the first term in the right-hand side of the first equation in (22) balanced.
What to read after Wave Propagation Across Ion Cyclotron Resonance Harmonic Layers?
You can find similar books in the "Read Also" column, or choose other free books by Kaya Imre to read onlineMoreLess
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