2021
DOI: 10.1109/tap.2021.3061011
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Omnidirectional Circularly Polarized Antenna Based on Counter-Wound Helices

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Cited by 14 publications
(15 citation statements)
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“…Thus, it is relatively easy to achieve circular polarization in a structure such as the λ /2 helix shown in Figure 3A. However, the problem is that its input resistance near the resonant frequency, f 0 , is very small due to the small antenna volume in Reference [19], rendering it less attractive for use as an OCP antenna or an array element. One viable way to obtain a larger resistance is to increase the antenna size.…”
Section: Operation Principlementioning
confidence: 99%
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“…Thus, it is relatively easy to achieve circular polarization in a structure such as the λ /2 helix shown in Figure 3A. However, the problem is that its input resistance near the resonant frequency, f 0 , is very small due to the small antenna volume in Reference [19], rendering it less attractive for use as an OCP antenna or an array element. One viable way to obtain a larger resistance is to increase the antenna size.…”
Section: Operation Principlementioning
confidence: 99%
“…In case S 1 and S 2 are equal, the condition of circular polarization can be easily derived, following Reference [20], as s1λgoodbreak=πD2λ2 In case S 1 and S 2 are not identical, circular polarization can still be achieved when the total vertical and horizontal components of far‐zone electric fields are equal. Following Reference [19], the CP condition can be approximately formulated as n1s1+2n2s2λgoodbreak=()n1goodbreak+2n2πD2λ2 Note that the thickness of helical wires and edge effect are not considered in Equation (). It is meant to estimate the initial values of the antenna parameters.…”
Section: Operation Principlementioning
confidence: 99%
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