Read e-book online Radar Target Imaging PDF

Nonfiction 8

By H. Überall (auth.), W.-M. Boerner, H. Überall (eds.)

ISBN-10: 3642851126

ISBN-13: 9783642851124

ISBN-10: 3642851142

ISBN-13: 9783642851148

Radar imaging, as understood right here, includes aim acceptance, i.e. the decision of the exact homes of an item (size, form, constitution and composition, and likewise place and pace) from radar echoes back by way of it. complicated ways are required for this, and several other of modern curiosity are mentioned during this ebook. They contain mathematical inverse-scattering strategies in accordance with the answer of critical equations; use of the singularity growth technique (SEM), regarding the resonance scattering idea (RST), during which the trend of resonance-frequency position within the complicated frequency aircraft might be hired to symbolize a given radar objective; and using polarization details. ultimately, the dimension of radar cross-sections is described.

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Extra resources for Radar Target Imaging

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16 represents an optimum receiver for polarization-based disturbance cancellation: it implements the above-described optimum procedure. In such a scheme, CHS means change sign, alb means division, and the double frame box is used to indicate an operation giving rise to a complex output. Some suboptimum procedures. 23]. It can be verified that their performances are characterized by a limited loss of cancellation ratio with respect to the optimum procedure, when the hypotheses made for this technique still hold.

1,4J, and is then seen to represent the reflected wave of Fig. 1; this calculation is not explicitly presented here. 5,6J as a tool for analyzing radar scattering phenomena in real time and in frequency space. 14a) , a=1 with complex amplitudes Ra and exponents Sa. 14b) , Sa where S = jw, and Wa = 1m Sa are the natural frequencies (eigenfrequencies) of the target. 14c) where r", = - 2 Resa is the full width at half maximum of the ath resonance. 14d) 52 H. Uberall The Laplace transform of the scattering amplitude thus has poles in the complex s plane (located in the second quadrant); equivalently, the Fourier transform has poles in the complex frequency (m) plane, located in the first quadrant.

Poelman: "On using orthogonally polarized noncoherent receiving channels to detect target echoes in Gaussian noise," IEEE Trans. c. Vannicola, S. Lis: "Polarization vector signal processing for Radar clutter suppression," in Inverse Methods in Electromagnetic Imaging, Part II, ed. M. Boerner et a!. (D. , Hingham, MA 1985) pp. L. Van Trees: Detection, Estimation and Modulation Theory, Part III (Wiley, New York, 1971) M. Born, E. R. Huynen, "Phenomenological theory of radar targets," in Electromagnetic Scattering, ed.

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Radar Target Imaging by H. Überall (auth.), W.-M. Boerner, H. Überall (eds.)

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