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The specular component is obtained by use of the Fresnel reflection coefficient and the creeping wave component from that for the perfectly co nducting body which is adjusted by means of a loss attenuation factor. The method is applied to the spher e and the resulting cross ections compare favorably witl~ those obtained using the exact solution. These methods can b e applied to smoot h bodiCs other than those of spherical shape and to dielectric-con stants other than zero provided the creeping wave component for the perfectly conducting body is known. The radar cross section of plasma bodies at a fre­ quency equal to the plasma frequency is controlled by means of the loss mechani m. The manner in which it is controlled is to be demonstrated in this paper by consideration of lossy homogeneous plasma spheres.

Radar cross sections of plasma bodies at the plasma frequency