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Inverse Synthetic Aperture Radar Imaging With MATLAB Algorithms, 2nd Edition
book

Inverse Synthetic Aperture Radar Imaging With MATLAB Algorithms, 2nd Edition

by Caner Ozdemir
May 2021
Intermediate to advanced
672 pages
16h 10m
English
Wiley
Content preview from Inverse Synthetic Aperture Radar Imaging With MATLAB Algorithms, 2nd Edition

2Radar Fundamentals

2.1 Electromagnetic Scattering

Scattering is the physical phenomenon that occurs when an electromagnetic (EM) wave hits a discontinuity/nonuniformity or an object. The deviation of the reflected wave's trajectory or path is generally known as scattering.

The classification of scattering phenomena can be made according to the size of the scattering object (or the scatterer) with respect to the wavelength of the EM wave. Radar signals reflect or scatter in different forms depending on the wavelength of the EM wave and the shape of the object (scatterer). If the wavelength of the EM wave is much smaller than the size of the scatterer, the EM wave bounces back in a similar way to how light reflects from a large surface. This type of scattering is often called scattering in the optical region (Stover 1995). If the EM wave's wavelength is of comparable size of the scatterer, such as within a few wavelengths, some resonances may occur, and the scattering intensity may fluctuate considerably for different frequencies. The scattering direction is mainly affected by the incident wave direction in this region that is usually called Mie region (or resonant region). This particular scattering type is, therefore, called Mie scattering. If the wavelength of the EM wave is much longer than the size of the scatterer, the wave is dispersed around the scatterer. This type of reflection is named as Rayleigh scattering (Brummund and Mesnier 1999; Zhong‐Cai et al. 2006).

Scattering ...

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ISBN: 9781119521334Purchase Link