1943
DOI: 10.1109/jrproc.1943.230327
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Optimum Current Distributions on Vertical Antennas

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1965
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Cited by 24 publications
(2 citation statements)
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“…The far-field pattern function is now more clearly related to the 2D Fourier transform of the current density pattern Π θ over the unit sphere. The far-field expression (10) indicates that there are no dc components of the source excitation radiated into the far field and that the radial dependence is that of a spherical wave. The Fourier transform integral determines if there are any preferred directions into which the fields are radiated.…”
Section: Needle Radiation From Currents On a Small Spherementioning
confidence: 99%
See 1 more Smart Citation
“…The far-field pattern function is now more clearly related to the 2D Fourier transform of the current density pattern Π θ over the unit sphere. The far-field expression (10) indicates that there are no dc components of the source excitation radiated into the far field and that the radial dependence is that of a spherical wave. The Fourier transform integral determines if there are any preferred directions into which the fields are radiated.…”
Section: Needle Radiation From Currents On a Small Spherementioning
confidence: 99%
“…Both end-fire (maximum radiated power is oriented along the array direction) [8] and broadside (maximum radiated power is oriented perpendicular to the plane of the array) [9] pattern enhancements from different array configurations were considered initially. La Paz and Miller [10] purported to show that the maximum directivity from an aperture of a given size was fixed, but Bouwkamp and De Bruijn [11] correctly demonstrated that there was no theoretical limit on the directivity from an aperture of any size. Dolph realized that one could control the sidelobe levels of the pattern by properly weighting (Chebyshev polynomial tapering) the amplitudes of the element excitations [12].…”
Section: Introductionmentioning
confidence: 99%