Hostname: page-component-848d4c4894-ndmmz Total loading time: 0 Render date: 2024-05-27T00:25:14.373Z Has data issue: false hasContentIssue false

The edge conditions and field representation theorems in the theory of electromagnetic diffraction

Published online by Cambridge University Press:  24 October 2008

A. E. Heins
Affiliation:
Carnegie Institute of Technology†Pittsburgh, Pennsylvania
S. Silver
Affiliation:
University of CaliforniaBerkeley, California

Extract

In 1897 Rayleigh(14) pointed out that it is possible to obtain a family of solutions to certain problems in diffraction theory, notably those involving plane obstacles, by the simple operation of differentiation of some one solution. This, of course, alters the nature of the solution, especially so in the neighbourhood of a sharp edge. For, at an edge the parent solution may be finite and yet its derivative can become infinite. Further, such a differentiated solution may produce an infinite total energy in the neighbourhood of the edge. It is, therefore, natural to ask what conditions are required to make the solutions of these problems physically and mathematically acceptable and thus define the boundary-value problem uniquely.

Type
Research Article
Copyright
Copyright © Cambridge Philosophical Society 1955

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

(1)Booker, H. J.Instn elect. Engrs, 93, part III A (1946), 620.Google Scholar
(2)Bouwkamp, C. J.Physica, 's Grav., 12 (1946), 467.CrossRefGoogle Scholar
(3)Bouwkamp, C. J.Math. Rev. 8 (1947), 180.Google Scholar
(4)Copson, E. T.Proc. roy. Soc. A, 186 (1946), 100.Google Scholar
(5)Copson, E. T.Admiralty Computing Service Report (1946).Google Scholar
(6)Jones, D. S.Quart. J. Mech. 3 (1950), 420.CrossRefGoogle Scholar
(7)Jones, D. S.Quart. J. Mech. 5 (1952), 363.CrossRefGoogle Scholar
(8)Jones, D. S.Proc. Lond. math. Soc. (3), 2 (1952), 440.CrossRefGoogle Scholar
(9)Jones, D. S.Proc. Camb. phil. Soc. 48 (1952), 733.CrossRefGoogle Scholar
(10)Kellogg, O. D.Foundations of potential theory (Berlin, 1929).CrossRefGoogle Scholar
(11)Maue, A. W.Z. Phys. 126 (1949), 601.CrossRefGoogle Scholar
(12)Meixner, J.Ann. Phys., Lpz., 6 (1949), 1.Google Scholar
(13)Muller, C.Abh. dtsch. Akad. Wiss. Berl. 3 (1945/1946).Google Scholar
(14)Rayleigh, Lord. Phil. Mag. 43 (1897), 259.CrossRefGoogle Scholar
(15)Schmeidler, W.Integralgleichungen mit Anwendungen in Physik und Technik (Leipzig, 1950).Google Scholar
(16)Silver, S.Microwave antenna theory and design (New York, 1949).Google Scholar
(17)Stratton, J. A.Electromagnetic theory (New York, 1941).Google Scholar