scholarly journals XI. The electrification of two parallel circular discs

The only problem relating to two electrified circular discs, placed parallel to each other, for which an exact solution has been obtained hitherto, is the classical one of Nobili’s rings. This was solved by Riemann,* by an application of the Bessel-Fourier integral method. In this problem the discs are circular electrodes fixed to two infinite conducting planes, which are themselves connected together by the earth or by a wire at infinity. If the axis of z is that of the two co-axial discs, and perpendicular to the infinite plane conducting sheets, the electrical potential V satisfies Laplace’s equation at all points between the plates, and the further conditions (1) ∂V/∂ z = 0, z = ± a , p > p 1 (2) ∂v/∂ z = A/√(r 1 2 —r 2 ), z = ± a , p < p 1 where A is a constant, 2 a is the distance between the plates, bisected by the origin, p 1 is the radius of either disc, and p is the distance of any point from the axis of z . In fact ( z , p ) are the two cylindrical polar co-ordinates on which V can alone depend.

In the course of a preliminary investigation of fluid motion when viscosity is taken into account, it was found that a solution of Laplace’s equation was obtained in very general form. The solution gives exact analytical expressions where the conditions of the problem admit of exact solution, but the chief claim to notice arises from the extremely general character of the method if graphical and mechanical integration are employed. The problem has been approached from the engineering standpoint, and the absence of any proof of the convergency of the series developed will immediately he evident to the mathematician. The justification by trial in particular cases is all that is attempted at the present moment, but in those cases the result is wholly satisfactory. For the analytical solution of the problems I am indebted to Mr. Arthur Berry who has added a second part to this paper, and has generally acted as helpful critic.


1965 ◽  
Vol 32 (3) ◽  
pp. 637-642 ◽  
Author(s):  
C. C. Mow

The transient response of a rigid spherical inclusion of arbitrary density embedded in an elastic medium owing to an incident pulse is examined in this paper. The Fourier-integral method is used, and an exact solution of the response is obtained. It is found that the acceleration and velocity of the inclusion are substantially different from those of the medium. A slight difference in the time history of the displacement between the inclusion and the medium is also noted.


1984 ◽  
Vol 33 (3) ◽  
pp. 205-207 ◽  
Author(s):  
N. M. Miskovsky ◽  
P. H. Cutler ◽  
T. E. Feuchtwang

1950 ◽  
Vol 2 (1) ◽  
pp. 23-33 ◽  
Author(s):  
John W. Miles

SummaryA linearised theory for the subsonic, lifting surface problem is formulated in terms of Fourier integral solutions to Laplace’s equation. The symmetric and anti-symmetric problems of the first kind are solved explicitly, while the problems of the second kind depend on the solution of dual integral equations. The antisymmetric problem of the second kind is cast in a variational form, from which certain well-known theorems may be deduced.


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