The Diffraction of Oblique Surface Waves By a Right Angle Bend
The Diffraction of Oblique Surface Waves By a Right Angle Bend
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To quickly assess the difficulty of the text, read a short excerpt:
A)a|.^/3''p^a), . , „, ] (4. 40; J>'f (K?)d| ^1 . 2 Now the explicit expressions for the six coefficients k, R, A, B, B^, and C^ have been obtained in the six equations, (4. 34), (4.^35), (4. 40), (4. 27), (4. 38) and (4. 25) respectively. This observation completes the formal solution of this case.
It is of interest to determine the far-zone forms of the radiated field. We first w ite down the asymptotic forms of the functions f and g.
(4. 41) f 1 v JtKr ■f ll«^ [^ i(Kr-— ) ^ (4. 42) g ~ e iko.... S' The far- zone forms of \|/ and f are expected to be (4. 43) M (cp) ^ iHcr + ik^. S' VT 18 (k. Hk) ^ = COS4) ^ - - smcp g;: ~ coscp^ .
Substituting Egs. (UAl), (k. HS) and (U. U) into Eq. (h. L'^) gives (^•^5) 1^1 = i. Cos cp-a^ y^ ^ [^1 sin ^ cp e + A^sin rcpe Substituting Eqs. {k. K2), {h. K3) and (h. Kk) into Eq. (U. L8) gives (^•^6) ^2= i. Cosc^-a, sl-^r ' ^BpSin f cp e 12, ^^3^, ^^, 12 J ^ Then substituting the above two expressions into Eq. . (^-^O) yields ih. Hl) E = T-r-^ 7 / -^ e -^^ ^' '-/^ ^^-- Lsin |cp +A^sin ^cpe ^ 1 r 2 1| "^^1 ^ iK cos cp -a^ [\-- I ^ -^^2^^- 3 ^^ J rr- KKr-g^-k S')f a \ 2 U -ifl (1+.
What to read after The Diffraction of Oblique Surface Waves By a Right Angle Bend?
You can find similar books in the "Read Also" column, or choose other free books by Samuel Karp to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
A)a|.^/3''p^a), . , „, ] (4. 40; J>'f (K?)d| ^1 . 2 Now the explicit expressions for the six coefficients k, R, A, B, B^, and C^ have been obtained in the six equations, (4. 34), (4.^35), (4. 40), (4. 27), (4. 38) and (4. 25) respectively. This observation completes the formal solution of this case.
It is of interest to determine the far-zone forms of the radiated field. We first w ite down the asymptotic forms of the functions f and g.
(4. 41) f 1 v JtKr ■f ll«^ [^ i(Kr-— ) ^ (4. 42) g ~ e iko.... S' The far- zone forms of \|/ and f are expected to be (4. 43) M (cp) ^ iHcr + ik^. S' VT 18 (k. Hk) ^ = COS4) ^ - - smcp g;: ~ coscp^ .
Substituting Egs. (UAl), (k. HS) and (U. U) into Eq. (h. L'^) gives (^•^5) 1^1 = i. Cos cp-a^ y^ ^ [^1 sin ^ cp e + A^sin rcpe Substituting Eqs. {k. K2), {h. K3) and (h. Kk) into Eq. (U. L8) gives (^•^6) ^2= i. Cosc^-a, sl-^r ' ^BpSin f cp e 12, ^^3^, ^^, 12 J ^ Then substituting the above two expressions into Eq. . (^-^O) yields ih. Hl) E = T-r-^ 7 / -^ e -^^ ^' '-/^ ^^-- Lsin |cp +A^sin ^cpe ^ 1 r 2 1| "^^1 ^ iK cos cp -a^ [\-- I ^ -^^2^^- 3 ^^ J rr- KKr-g^-k S')f a \ 2 U -ifl (1+.
What to read after The Diffraction of Oblique Surface Waves By a Right Angle Bend?
You can find similar books in the "Read Also" column, or choose other free books by Samuel Karp to read onlineMoreLess
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