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Introduction

  • Roger A. Dana
Chapter

Abstract

First the assumptions and limitations of the k-space gain formulation are enumerated. These include the assumption of observing the gain in the far field of the array, the demarcation of which is explained further in Appendix 1. Next are descriptions of antenna performance metrics used to evaluate performance: peak gain, maximum sidelobe level, beamwidths, and integrated sidelobe level (ISL). Then it is shown that plane waves are solutions of Maxwell’s equations (or more specifically, of the Helmholtz wave equation). This is a key result since the k-space gain formulation is based on two-dimensional (2-D) expansions of the ESA spatial weighting function into the summation of plane waves, each with its own amplitude and phase, through continuous or discrete 2-D Fourier transforms.

Keywords

Near field Plane waves Maxwell’s equations Helmholtz wave equation Fourier transforms Electronically scanned array 

References

  1. Jackson, J. D. (1962). Classical electrodynamics. New York: Wiley.zbMATHGoogle Scholar
  2. Stratton, J. A. (1941). Electromagnetic theory. New York: McGraw-Hill Book Company.zbMATHGoogle Scholar
  3. Taylor, T. T. (1955, January). Design of line source antenna for narrow beam width and low side lobes. IRE Transactions on Antennas and Propagation, 3, 16–28.CrossRefGoogle Scholar

Copyright information

© Springer Nature Switzerland AG 2019

Authors and Affiliations

  • Roger A. Dana
    • 1
  1. 1.Advanced Technology Center of Rockwell CollinsCedar RapidsUSA

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