Basic Mathematical Investigations in Electromagnetic Wave Theory Final Report
Basic Mathematical Investigations in Electromagnetic Wave Theory Final Report
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In our eReader you can find the full English version of the book. Read Basic Mathematical Investigations in Electromagnetic Wave Theory Final Report 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 Basic Mathematical Investigations in Electromagnetic Wave Theory Final Report
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The solution u of a wave propagation problem for the medium a depends upon a. Therefore it is denoted by u(a) and with it is associated the probability distribution p(a). This makes u(a) a random wave. Then the mean value of any functional F[u] is denoted by and is defined by (1) = F[u(a)]p(a)da.
It is assumed that certain statistical properties of the wave in the 30 random medium will correspond to properties of the wave in a given com- plex medium, provided that the random medium is chosen ...appropriately to model that medium.
In a general way the problem and the basic methods employed in reports EM-208, 210 and 231 may be formulated as follows. Let it be assumed that in the medium a, the state of the system u(a) = u(x, t;a), a vector function of space and time, (2) L(a)u = g where L(a) is a linear operator depending on a, and g is a given non- random function. If L(a) is invertible, as we assume it to be for almost all a, we may write the solution of (1) as u(a) = L (a)g.
What to read after Basic Mathematical Investigations in Electromagnetic Wave Theory Final Report?
You can find similar books in the "Read Also" column, or choose other free books by Joseph B Keller to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
The solution u of a wave propagation problem for the medium a depends upon a. Therefore it is denoted by u(a) and with it is associated the probability distribution p(a). This makes u(a) a random wave. Then the mean value of any functional F[u] is denoted by
It is assumed that certain statistical properties of the wave in the 30 random medium will correspond to properties of the wave in a given com- plex medium, provided that the random medium is chosen
In a general way the problem and the basic methods employed in reports EM-208, 210 and 231 may be formulated as follows. Let it be assumed that in the medium a, the state of the system u(a) = u(x, t;a), a vector function of space and time, (2) L(a)u = g where L(a) is a linear operator depending on a, and g is a given non- random function. If L(a) is invertible, as we assume it to be for almost all a, we may write the solution of (1) as u(a) = L (a)g.
What to read after Basic Mathematical Investigations in Electromagnetic Wave Theory Final Report?
You can find similar books in the "Read Also" column, or choose other free books by Joseph B Keller to read onlineMoreLess
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