Electromagnetic scattering interaction between a dielectric cylinder and a slightly rough surface

An electromagnetic scattering solution for the interaction between a dielectric cylinder and a slightly rough surface is presented in this paper. Taking the advantage of a newly developed technique that utilizes the reciprocity theorem, the difficulty in formulating the secondary scattered fields from the composite target reduces to the evaluation of integrals involving the scattered fields from the cylinder and polarization currents of the rough surface induced by a plane wave. Basically, only the current distribution of isolated scatterers are needed to evaluate the interaction in the far-field region. The scattered field from the cylinder is evaluated in the near-field region using a stationary phase approximation along the cylinder axis. Also, the expressions for the polarization current induced within the top rough layer of the rough surface derived from the iterative solution of an integral equation are employed in this paper. A sensitivity analysis is performed for determining the dependency of the scattering interaction on the target parameters such as surface root mean square (RMS) height, dielectric constant, cylinder diameter, and length. It is shown that for nearly vertical cylinders, which is of interest for modeling of vegetation, the cross-polarized backscatter is mainly dominated by the scattering interaction between the cylinder and the rough surface. The accuracy of the theoretical formulation is verified by conducting polarimetric backscatter measurements from a lossy dielectric cylinder above a slightly rough surface. Excellent agreement between the theoretical prediction and experimental results is obtained.

[1]  F. Ulaby,et al.  Radar polarimetry for geoscience applications , 1990 .

[2]  Kamal Sarabandi,et al.  Electromagnetic scattering from slightly rough surfaces with inhomogeneous dielectric profiles , 1997 .

[3]  S. Rice Reflection of electromagnetic waves from slightly rough surfaces , 1951 .

[4]  F. Ulaby,et al.  Microwave Dielectric Behavior of Wet Soil-Part 1: Empirical Models and Experimental Observations , 1985, IEEE Transactions on Geoscience and Remote Sensing.

[5]  Stephen L. Durden,et al.  Modeling and observation of the radar polarization signature of forested areas , 1989 .

[6]  Kamal Sarabandi,et al.  A Convenient Technique For Polarimetric Calibration Of Radar Systems , 1990, 10th Annual International Symposium on Geoscience and Remote Sensing.

[7]  Polarimetric backscattering measurements of herbaceous vegetation: a sensitivity study for soil moisture retrieval , 1996, IGARSS '96. 1996 International Geoscience and Remote Sensing Symposium.

[8]  Fawwaz Ulaby,et al.  Microwave Dielectric Spectrum of Vegetation - Part II: Dual-Dispersion Model , 1987, IEEE Transactions on Geoscience and Remote Sensing.

[9]  F. Ulaby,et al.  A convenient technique for polarimetric calibration of single-antenna radar systems , 1990 .

[10]  J. Kong,et al.  Theory of microwave remote sensing , 1985 .

[11]  Kamal Sarabandi,et al.  Electromagnetic scattering from short branching vegetation , 2000, IEEE Trans. Geosci. Remote. Sens..

[12]  F. Ulaby,et al.  Monte Carlo simulation of scattering from a layer of vertical cylinders , 1993 .

[13]  R. Harrington Time-Harmonic Electromagnetic Fields , 1961 .

[14]  A. Schneider,et al.  Electromagnetic scattering from a dielectric cylinder of finite length , 1988 .

[15]  Kamal Sarabandi,et al.  A Monte Carlo coherent scattering model for forest canopies using fractal-generated trees , 1999, IEEE Trans. Geosci. Remote. Sens..

[16]  Kamal Sarabandi,et al.  Electromagnetic scattering from two adjacent objects , 1994 .

[17]  J. Kong,et al.  Radiative transfer theory for polarimetric remote sensing of pine forest at P band , 1994 .

[18]  Kamal Sarabandi,et al.  Michigan microwave canopy scattering model , 1990 .