초록 ▼

An apparatus for and a method of determining the material properties of a dielectric and/or conducting radar target by deciphering the backscattered signals returned from the target is disclosed. The resonance “code”of the echo signals from the target is a function of the width and spacing of the re

An apparatus for and a method of determining the material properties of a dielectric and/or conducting radar target by deciphering the backscattered signals returned from the target is disclosed. The resonance “code”of the echo signals from the target is a function of the width and spacing of the resonant spectral lines in the transverse electric (TE) and transverse magnetic (TM) modes of the returned signals. The resonances present in any TE or TM mode become uniformly spaced and of uniform width at high frequencies. The uniform spacing between adjacent resonances is used to uniquely determine the dielectric constant of the material comprising the target, and their uniform width is used to uniquely determine its thickness.

대표청구항 ▼

A method of determining the material properties of a target/obstacle comprising the steps of: directing electromagnetic energy in the form of incident wave pulses having a known frequency spectrum at said target/obstacle creating thereon, electromagnetic oscillations including a set of modal resonan

A method of determining the material properties of a target/obstacle comprising the steps of: directing electromagnetic energy in the form of incident wave pulses having a known frequency spectrum at said target/obstacle creating thereon, electromagnetic oscillations including a set of modal resonances superposed thereon; receiving a portion of said incident wave pulses backscattered from said target/obstacle and conditioning it into representative electrical signals; converting said electrical signals into an echo pattern (“radar cross-section”) of said target/obstacle, said echo pattern being a plot of squared scattering amplitudes versus normalized frequency; subdividing said echo pattern into its partial-wave resonance components, each corresponding to a particular resonance mode; determining the background components of said partial-wave resonance components, said background components being the resonance response of a perfectly conducting scatterer of the same size of said target/obstacle, and said background components being obtained from said partial-wave components by setting the modal impedances (Zn) and admittances (Yn) equal to zero (0) and infinity (∽), respectively; substracting each of said background components from each of said partial-wave resonance components of the same particular resonance mode, thereby isolating the resonances in the frequency spectrum which are the fundamental frequency and its overtones for each modal contribution; and measuring the asymptotic spacings between any two consecutive modal overtones and the asymptotic widths of any two consecutive modal overtones, said asymptotic spacings and said asymptotic widths being used to obtain the dielectric constant and the thickness of the coating layer covering the conducting core of said target/obstacle.