The book covers everything from the fundamental physics of radar scattering to real-world radar absorbent materials (RAM) and actual measurement range setups.
σ=limR→∞4πR2|Es|2|Ei|2sigma equals limit over cap R right arrow infinity of 4 pi cap R squared the fraction with numerator the absolute value of cap E sub s end-absolute-value squared and denominator the absolute value of cap E sub i end-absolute-value squared end-fraction = Distance from the radar to the target Escap E sub s = Scattered electric field strength at the receiver Eicap E sub i = Incident electric field strength hitting the target
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Knott has authored 27 academic papers, which have received over 1,500 citations. His research spans across . He has collaborated with other giants in the field, such as T. B. A. Senior and Valdis V. Liepa, and has been published in the most prestigious journals, including the Proceedings of the IEEE and IEEE Transactions on Antennas and Propagation .
: Detailed mathematical methods for calculating RCS for simple shapes like spheres and cylinders. High-Frequency RCS Prediction The book covers everything from the fundamental physics
Managing how radar waves bounce between different parts of a target. Factors Affecting RCS
The physical book’s index is exhaustive, but the PDF version (if properly OCR’d) is interactive. You can jump from "Stealth" to "Swerling Targets" to "Polarization Scattering Matrix" in seconds. For a working engineer debugging a radar threat library, this responsiveness is invaluable. Let me point you to the definitive answer:
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σdBsm=10log10(σm2)sigma sub dBsm end-sub equals 10 log base 10 of open paren the fraction with numerator sigma and denominator m squared end-fraction close paren Why the Eugene F. Knott Text is the Gold Standard
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