Abstract
A long circular cylinder of radius
a
, with its axis horizontal, is half-immersed in a fluid under gravity and is making periodic vertical oscillations of small constant amplitude and of period 2
π
/σ about this position. It is required to find the resulting fluid motion when the parameter
N
= σ
2
a
/
g
is large; the method of an earlier paper (Ursell 1949) is then unworkable. The present solution is made to depend on an integral equation (3∙15) which can be chosen to have a kernel tending to zero with
N
-1
, and which is solved by iteration. Successive terms in the iteration are of decreasing order, and the convergence of the method for sufficiently large
N
is proved. Expressions are given for the virtual-mass coefficient (5∙1) and for the wave amplitude at infinity (5∙7). The present work appears to be the first practical and rigorous solution of a short-wave problem when a solution in closed form is not available. It is suggested that a similar technique may be applicable to the diffraction problems of acoustics and optics, which have hitherto been treated by the approximate Kirchhoff-Huygens principle.
Reference3 articles.
1. B ak er B. B. & Copson E . T . 1950 O xford U n IV ersity Press.
2. H avelock T. H . 1929 P h il. M ag. (7) 8 569.
3. H ellinger E . & T oeplitz O. 1927 3. Teil 2. H alfte . L e ip z ig : T eubner. Them athem atical theory o f H u yg en s' p rin cip le 2n d ed.
Cited by
60 articles.
订阅此论文施引文献
订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献