Novel differential formulation of electromagnetic scattering by dielectric cylinders of arbitrary cross-section

1994 ◽  
Vol 141 (3) ◽  
pp. 189 ◽  
Author(s):  
H. Tosun
Keyword(s):  
Cross Section ◽  
Electromagnetic Scattering ◽  
Arbitrary Cross Section ◽  
Differential Formulation

Electromagnetic Scattering by a Moving Conducting Cylinder of Arbitrary Cross Section

1973 ◽  
Vol 51 (22) ◽  
pp. 2389-2394 ◽  
Author(s):  
J. D. Hunter
Keyword(s):  
Cross Section ◽  
Electromagnetic Scattering ◽  
Incident Field ◽  
Arbitrary Cross Section ◽  
Square Cylinder ◽  
Field Source ◽  
Conducting Cylinder ◽  
Arbitrary Velocity

A method is derived for calculating the electromagnetic scattering from a conducting cylinder of arbitrary cross section moving with arbitrary velocity relative to the field source and the observer. Results are presented for a moving square cylinder for both TM and TE polarizations of the incident field.

ELECTROMAGNETIC SCATTERING FROM CYLINDERS OF ARBITRARY CROSS‐SECTION IN A CONDUCTIVE HALF‐SPACE

Geophysics ◽  
1971 ◽  
Vol 36 (1) ◽  
pp. 67-100 ◽  
Author(s):  
J. R. Parry ◽  
S. H. Ward
Keyword(s):  
Half Space ◽  
Cross Section ◽  
Electromagnetic Scattering ◽  
Numerical Technique ◽  
Surface Current ◽  
Arbitrary Cross Section ◽  
Integral Representations ◽  
Radius Of Curvature ◽  
Current Densities ◽  
Conducting Cylinders

A general numerical technique is presented for solving the problem of electromagnetic scattering by conducting cylinders of arbitrary cross‐section located in a conductive half‐space. Solutions to the electromagnetic wave equation are required for the free space above the half‐space, for the half‐space surrounding the cylinder, and for the cylinder. The problem is formulated by choosing an integral representation for the electromagnetic fields in each of the three homogeneous regions. By enforcing the boundary conditions on tangential E and H, we obtain a set of coupled integral equations which can be solved numerically for the unknown equivalent surface current densities on the interface bounding each homogeneous region. Once these current densities have been estimated, the fields can be calculated at any point from the general integral representations. The following conclusions are among those of importance to AFMAG and VLF surveys: 1) the ratio of Re (H) to Im (H) is a function of traverse position and of ground conductivity, as well as of cylinder conductivity and of survey frequency; 2) in no case was a zero phase observed, even for perfectly conducting cylinders; and 3) reverse crossovers in Im (H) can occur in the field scattered by a single conductor whenever the radius of curvature on the upper portion of a “poor” conductor is small.

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