2019
DOI: 10.1109/maes.2019.2916537
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An Overview of Radomes for Large Ground-Based Antennas

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Cited by 12 publications
(6 citation statements)
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“…The attenuations are to be considered when the radome thickness th (i.e., in the specialized literature, the radome thickens is abbreviated by the t symbol; however, to not be confused with time notation, this study will use th instead) is on the same scale with the communication wavelength λ. However, when th is much smaller than λ , the induced losses are sub-unitary [ 54 , 55 , 56 ]. In this study, the plastic lid thickness is 1 mm, while th represents the 2 cm distance of the Rx antenna to the lid; therefore, for the testing λ of 0.345 and 0.124 m, the lid-induced losses can be neglected since the weather during experiments was dry (i.e., without inducing water accumulations on the lid area).…”
Section: Methodsmentioning
confidence: 99%
“…The attenuations are to be considered when the radome thickness th (i.e., in the specialized literature, the radome thickens is abbreviated by the t symbol; however, to not be confused with time notation, this study will use th instead) is on the same scale with the communication wavelength λ. However, when th is much smaller than λ , the induced losses are sub-unitary [ 54 , 55 , 56 ]. In this study, the plastic lid thickness is 1 mm, while th represents the 2 cm distance of the Rx antenna to the lid; therefore, for the testing λ of 0.345 and 0.124 m, the lid-induced losses can be neglected since the weather during experiments was dry (i.e., without inducing water accumulations on the lid area).…”
Section: Methodsmentioning
confidence: 99%
“…A well-known technique to reduce the scattering of radome seams is to integrate metallic structures, such as wires or grids, within the volume of the dielectric seam, which is then said to be tuned [1][2][3][4]. The scattering reduction induced by these metallic structures can be explained in terms of internal current redistribution phenomena within the dielectric volume [1].…”
Section: Introductionmentioning
confidence: 99%
“…[ 1–10 ] Plasmonic cloaking of dielectric spheres and cylinders can be achieved by enveloping the object with a dielectric coat, whose permittivity needs to be carefully engineered. [ 1–21 ] The realization of such cloaks requiring specific anisotropic material properties is often technologically challenging and is more inclined to losses due to the bulky nature of the cloak. Moreover, the addition of a bulky cloak inevitably increases the profile of the scatterer, which may not always be compatible with specific applications of the scatterer.…”
Section: Introductionmentioning
confidence: 99%
“…Such tuning techniques are thus, by definition, invasive and require the modification of the dielectric volume, in clear opposition to cloaking techniques that require an external cloak and do not inherently modify the scatterer. While wire‐tuning is a well‐known technique to reduce scattering from dielectric mechanical pieces, [ 11–14 ] the scattering reduction phenomenon is only effective when the electric field is parallel to the wires, clearly limiting the effectiveness of this solution for different polarizations of the impinging wave. This problem can be alleviated by using polarization‐insensitive grids instead of wires, but which are usually not optimized with respect to operating frequency and often rely on trial and error optimization procedures.…”
Section: Introductionmentioning
confidence: 99%