Theory of Long Period Magnetic Pulsations
Theory of Long Period Magnetic Pulsations
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In our eReader you can find the full English version of the book. Read Theory of Long Period Magnetic Pulsations 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 Theory of Long Period Magnetic Pulsations
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In the region II, Eq. (3. 24) becomes where a = k = kxd A^ - — 19 We now solve Eq. (3. 28) by means of the WKB method. For the range of the variable if such that 1^^ — a^ :7"^ 0, we transform ( to Za (-a ^ + Q and therefore we have dt] = d( -{e{r, )-a'y6 = 0.
(3. 29) Then Eq. (3. 22) is transformed to drj^ For (f^ not near q^, the WKB method yields the asymptotic solution of Eq. (3. 29) in terms of ^ as 6 = A+ {e - a'y'^\xpi + A. {e - a^y''' exp{-0. (3. 30) The boundary conditions to be applied... at z = ±(f are that the normal velocity viy{y) and the normal component of the stress pi + BqBiz be continuous. Since u>'{y) = u — kxVo{y) is continuous a± z = ±d, the continuous normal velocity conditions are [^]. =±. = 0, (3. 31) where [ ]^ indicates the change in the value of the enclosed quantity across the discontinuity surface at z. Since Eq. (3. 23) may be written as . Pu)' dS (pi + BoBu) = -i- kx dy' the continuous normal stress conditions are given by = 0.
d( (3. 32) Equation (3.
What to read after Theory of Long Period Magnetic Pulsations?
You can find similar books in the "Read Also" column, or choose other free books by Satoshi Hamaguchi to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
In the region II, Eq. (3. 24) becomes where a = k = kxd A^ - — 19 We now solve Eq. (3. 28) by means of the WKB method. For the range of the variable if such that 1^^ — a^ :7"^ 0, we transform ( to Za (-a ^ + Q and therefore we have dt] = d( -{e{r, )-a'y6 = 0.
(3. 29) Then Eq. (3. 22) is transformed to drj^ For (f^ not near q^, the WKB method yields the asymptotic solution of Eq. (3. 29) in terms of ^ as 6 = A+ {e - a'y'^\xpi + A. {e - a^y''' exp{-0. (3. 30) The boundary conditions to be applied... at z = ±(f are that the normal velocity viy{y) and the normal component of the stress pi + BqBiz be continuous. Since u>'{y) = u — kxVo{y) is continuous a± z = ±d, the continuous normal velocity conditions are [^]. =±. = 0, (3. 31) where [ ]^ indicates the change in the value of the enclosed quantity across the discontinuity surface at z. Since Eq. (3. 23) may be written as . Pu)' dS (pi + BoBu) = -i- kx dy' the continuous normal stress conditions are given by = 0.
d( (3. 32) Equation (3.
What to read after Theory of Long Period Magnetic Pulsations?
You can find similar books in the "Read Also" column, or choose other free books by Satoshi Hamaguchi to read onlineMoreLess
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