DocumentCode
1044801
Title
Realation between a class of two-dimensional and three dimensional diffraction problems
Author
Felsen, L.B. ; Karp, S.N.
Author_Institution
Polytechnic Institute of Brooklyn, Brooklyn, NY, USA
Volume
8
Issue
4
fYear
1960
fDate
7/1/1960 12:00:00 AM
Firstpage
407
Lastpage
414
Abstract
By means of a certain transformation, a relationship is demonstrated between a class of two-dimensional and three-dimensional scalar or electromagnetic diffraction problems. The basic three-dimensional configuration consists of a perfectly reflecting half plane excited by a ring source centered about the edge and having a variation exp (
), where
, is the azimuthal variable; in addition, a perfectly reflecting rotationally, symmetric obstacle whose surface is defined by
(
are cylindrical coordinates) may be superposed about the edge (
axis). This problem is shown to be simply related to the two-dimensional problem for the line source excited configuration
, where
and
are Cartesian coordinates. Various special obstacle configurations are treated in detail. For the general case of arbitrary electromagnetic excitation, the above-mentioned transformation is used to construct the solution for the diffraction by a perfectly conducting half plane from the knowledge of appropriate scalar solutions, namely those which obey the same equations and boundary conditions, and have the same excitations, as the Cartesian components of the electromagnetic field.
), where
, is the azimuthal variable; in addition, a perfectly reflecting rotationally, symmetric obstacle whose surface is defined by
(
are cylindrical coordinates) may be superposed about the edge (
axis). This problem is shown to be simply related to the two-dimensional problem for the line source excited configuration
, where
and
are Cartesian coordinates. Various special obstacle configurations are treated in detail. For the general case of arbitrary electromagnetic excitation, the above-mentioned transformation is used to construct the solution for the diffraction by a perfectly conducting half plane from the knowledge of appropriate scalar solutions, namely those which obey the same equations and boundary conditions, and have the same excitations, as the Cartesian components of the electromagnetic field.Keywords
Electromagnetic diffraction; Antennas and propagation; Boundary conditions; Electromagnetic diffraction; Electromagnetic fields; Electromagnetic propagation; Electromagnetic scattering; Equations; Receiving antennas; Wave functions;
fLanguage
English
Journal_Title
Antennas and Propagation, IRE Transactions on
Publisher
ieee
ISSN
0096-1973
Type
jour
DOI
10.1109/TAP.1960.1144860
Filename
1144860
Link To Document