On the Electromagnetic Field Equations in the Ionosphere
On the Electromagnetic Field Equations in the Ionosphere
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In our eReader you can find the full English version of the book. Read On the Electromagnetic Field Equations in the Ionosphere 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 On the Electromagnetic Field Equations in the Ionosphere
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Explicitly we introduce the new variables U(z) as in equations (2. 8) with U (2. 13) U(z) = ^, (z) ^2(0 . -"2(2); . P(z)= "JZJu) rr-1 . P'MO= Jl^v. Hz) \ 1 Uj 1 u 1 1 \ u \ 1 -y rr-l, The quantity u(z), as yet unspecified, is determined by the condition that P AP Bhall have zero off-diagonal blocks (i. E.. That the coefficient matrix in the equation -12- for U(z) "be avich. That the Tmcoupling of the system is optimal under the given condit- ions), IVom tthe matrix (2. 10) and (2, 13) we find t...hat this condition reqiiires (2. 14) u2 + [M^ + 1 = Tliis equation has two solutions u and -• » where « = (^) - 7(^)^-1 (2. 15) The equation satisfied "by Tl(z) is given "by equation (2. 9) where, with the above choice of u(z).
0-100 T ■-^"(z) [2. 16) P"-^ AP = ' ^ xliz)!*" ^^ u 1-u 10 • du ♦ Here we have introduced the notation u = t~ and dz \?(z) = a+- = P-Va 1 — u — \^(z) = a + Yu = P - Jf = 1 - -A 10 10 ;-l J Tf T "-H ^Tbyt/f^F^cby; *^ This system of equations is coupled in a sli^tly more conrplicated manner than the previous system "but still has only one coupling coefficient.
What to read after On the Electromagnetic Field Equations in the Ionosphere?
You can find similar books in the "Read Also" column, or choose other free books by Herbert Bishop Keller to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
Explicitly we introduce the new variables U(z) as in equations (2. 8) with U (2. 13) U(z) = ^, (z) ^2(0 . -"2(2); . P(z)= "JZJu) rr-1 . P'MO= Jl^v. Hz) \ 1 Uj 1 u 1 1 \ u \ 1 -y rr-l, The quantity u(z), as yet unspecified, is determined by the condition that P AP Bhall have zero off-diagonal blocks (i. E.. That the coefficient matrix in the equation -12- for U(z) "be avich. That the Tmcoupling of the system is optimal under the given condit- ions), IVom tthe matrix (2. 10) and (2, 13) we find t...hat this condition reqiiires (2. 14) u2 + [M^ + 1 = Tliis equation has two solutions u and -• » where « = (^) - 7(^)^-1 (2. 15) The equation satisfied "by Tl(z) is given "by equation (2. 9) where, with the above choice of u(z).
0-100 T ■-^"(z) [2. 16) P"-^ AP = ' ^ xliz)!*" ^^ u 1-u 10 • du ♦ Here we have introduced the notation u = t~ and dz \?(z) = a+- = P-Va 1 — u — \^(z) = a + Yu = P - Jf = 1 - -A 10 10 ;-l J Tf T "-H ^Tbyt/f^F^cby; *^ This system of equations is coupled in a sli^tly more conrplicated manner than the previous system "but still has only one coupling coefficient.
What to read after On the Electromagnetic Field Equations in the Ionosphere?
You can find similar books in the "Read Also" column, or choose other free books by Herbert Bishop Keller to read onlineMoreLess
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