IEEE Transactions on Antennas and Propagation · 1996 · 78 citations · 17 references
EngineeringElectrical EngineeringAntennasElectromagneticsElectromagnetismElectric PotentialFar-field RegionsIntegral Equation FormulationsMaxwell's EquationsNear-field RegionsPlanar AntennasAntenna AnalysisCurrent Density DistributionFar-field ApproximationIntegral Form FormulationLoop AntennasMagnetic Vector PotentialNear-field Integral EquationsVector Potential
Assuming a known (constant) current distribution on the thin circular loop antenna of arbitrary radius in free space, an exact integration of the vector potential is performed without recourse to approximations. The only restrictions on the solution variables are that the observation point distance must be greater than the loop radius and that the polar angle must run between 0 and /spl pi/. The resulting vector potential infinite series solution possesses a real part composed of linear combinations of complete elliptic integrals of the first and second kind and an imaginary part composed of elementary functions. Thus, it is possible to obtain an exact solution which is valid everywhere that r>a and 0/spl les//spl theta//spl les//spl pi/. The electromagnetic field components of the constant current circular loop antenna are then determined by direct series differentiation. These solutions are valid in the near and induction fields, converging rapidly there, and are also valid in the far field, although many terms of the series are needed for convergence.
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