CHAPTER 11
CHAPTER 11RADAR CROSS SECTIONEugene F. KnottThe Boeing INTRODUCTIONA radar detects or tracks a target, and sometimes can identify it, only becausethere is an echo signal. It is therefore critical in the design and operation of radarsto be able to quantify or otherwise describe the echo, especially in terms of suchtarget characteristics as size, shape, and orientation. For that purpose the targetis ascribed an effective area called the radar cross section. It is the projected areaof a metal sphere which would return the same echo signal as the target had thesphere been substituted for the the echo of the sphere, however, which is independent of the viewingangle, the echoes of all but the simplest targets vary significantly with orienta-tion. As such, one must mentally allow the size of this fictitious sphere to vary asthe aspect angle of the target changes. As will be shown, the variation can bequite rapid, especially for targets many wavelengths in echo characteristics depend in strong measure on the size and nature ofthe target surfaces exposed to the radar beam.
the wave equation are, at best, guidelines for gauging other (approximate) meth-ods of computing scattered fields. An alternative approach is the solution of the integral equations governing the
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PHYSICS, MATHEMATICS UNIT 1: REAL ANALYSIS, Equation, Cylindrical wave equation, Wave Equation in Cylindrical, Wave Equation in Cylindrical Coordinates, Equation in cylindrical coordinates, Hilbert METHODS OF, Hilbert METHODS OF MATHEMATICAL PHYSICS Volume II Partial Differential Equations, Solution of the Partial Differential, Solution of the Partial Differential Equations, INTRODUCTION TO THE SPECIAL FUNCTIONS, INTRODUCTION TO THE SPECIAL FUNCTIONS OF MATHEMATICAL PHYSICS, Revision E By Tom Irvine, Wave