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IEEE Transactions on Antennas and Propagation
Volume 48 Number 9, September 2000
Table of Contents for this issue
Complete paper in PDF format
Laboratory Models Used in
the Investigation of Radio Wave Propagation in Irregular Structures
Ezekiel Bahar LifeFellow, IEEE
Page 1367.
Abstract:
A laboratory model first conceived by Wait to investigate radio
wave propagation in the perturbed environment of the earth-ionosphere waveguide
is described here. The construction of the laboratory model involves the exploitation
of the following fundamental invariant properties of Maxwell's equations and
the ability to physically simulate the appropriate boundary conditions including
the earth's curvature: 1) invariance of Maxwell's equations to size-wavelength
transformations permits the scaling down in size of the earth-ionosphere waveguide;
2) duality relationships between the electric and magnetic fields permits
the representation of the azimuthally independent TMn,o
modes excited by vertical dipoles in the earth ionosphere
waveguide by the TEn,o modes in rectangular
waveguides; 3) a perfectly conducting magnetic wall (where the tangential
component of the magnetic field vanishes) is simulated through the use of
imaging techniques; 4) to account for dissipation in the ionosphere, an equivalent
surface impedance boundary is simulated using a wall loading material with
a specific thickness and complex permittivity; and 5) to simulate the earth's
curvature in the rectangular waveguide, an especially fabricated dielectric
material with a prescribed permittivity height profile is used as the medium
of propagation in the interior of the waveguide. All five of the above artifices
have been employed in order to construct a scaled model of the earth-ionosphere
waveguide. However, one or a combination of them can be employed by researchers
today to construct laboratory models from which controlled experimental data
can be obtained to validate analytical and numerical solutions as well as
to provide insights for novel approaches to solve difficult propagation problems.
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