Dielectric Resonator Antennas: An Analysis

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Abstarct: In this paper we get an overview of the dielectric resonator antenna which replaced the simple form of antennas that were being used for the past ten years. These dielectric antenna have been of a great importance to the research work in antenna field as these have a great dielectric constant and higher Q factor than the other isotropic or directive antennas. Earlier these antennas were considered to be energy storage devices but in this paper we have made use of the DRA antennas as radiators. These antennas have been described with their features which separates them from ordinary antennas, the features include small size, high efficiency etc. The DRA are compared to micro strip antennas in this review paper. Basically this paper gives an idea about the evolution of directive resonator antennas and their applications and the different DRA antennas are compared.
Introduction
From the time of origination of dielectric resonator antennas, they were being used in microwave circuits like filters or oscillators and were being used as energy storage devices until a paper was published in 1983 which made people accepted that these could be used as antennas and radiators.
The DRA is a resonant antenna, fabricated from a low loss and high-permittivity dielectric ceramic material mounted on a ground plane and fed by a coaxial probe, a slot, a waveguide, or a micro strip line. The size of DRA is inversely proportional to dielectric constant of material and losses in the DRA are also inversely proportional to quality factor of material. As compared to the micro strip antenna, the DRA has a much wider impedance bandwidth ( 10 % for dielectric constant εr  10). This is because the micro strip antenna radiates only through the whol...

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...ation resistance of the antenna (Ω)
R_loss=loss resistance of the antenna (Ω)
For physically small antennas, the Wheeler cap method is highly preferred for measuring the radiation efficiency. According to this method, if a radiation shield is placed around the antenna so as to enclose the near fields of the antenna, the radiation resistance of the antenna is reduced to zero while the loss resistance and the stored energy remain the same as for the unshielded antenna. When covering the antenna with a metal cap, the radiation is suppressed and the input power (proportional to the input resistance) is equal to the power loss (proportional to the loss resistance). Without the cap, the input power is equal to the radiated power plus the power loss (input resistance + loss resistance). The radiation efficiency of the antenna can be obtained from these two parameters.

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