Abstract:This paper investigates the behavior of a dipole antenna near the perfect electric conductor, perfect magnetic conductor, and artificial magnetic conductor (AMC). The phase variations due to reflector reflection coefficient and the distance between antenna and reflector are analyzed, and their effect on the antenna radiation patterns are studied for different frequencies. The cause of a null occurrence in the broadside direction of radiation pattern when using the AMC (or HIS) as a reflector is explored. It is… Show more
“…These characteristics are also obtained by fractal FSSs, 20 combinations of other forms of unit cells, 21,22 and array of rotational symmetric square split ring resonators 23,24 . The band stop FSSs with linear reflection phase behave as good reflectors and thus, these have been assembled with planar antennas to enhance their gain 2,13 …”
Section: Introductionmentioning
confidence: 99%
“…FSSs are two‐ or three‐dimensional structures composed of large array of unit cells arranged in periodic or quasiperiodic fashion to exhibit these characteristics for a desired frequency, multiple frequencies when illuminated by the EM waves 1 . The band stop or band pass filtering characteristics of FSSs have been explored for various applications such as artificial magnetic conductors (AMCs), 2,3 reflectors, 4 absorbers, 5 radomes, 6 and EM shields 7,8 and so forth. Based on symmetry of unit cells toward incident EM waves, the FSSs can either be polarization dependent or independent.…”
Dual rhombic loop (DRL) based low‐cost X‐band frequency selective surfaces (FSSs) with stopband characteristics are presented in this study. Orthogonally oriented arrays of rhombic loop pairs are printed back‐to‐back (BTB) on both sides of dielectric substrate to achieve wide stopband characteristics with stable response under oblique incidences. The nonlinearities in the reflection phase of BTB DRL printed FSSs are compensated by printing orthogonally oriented rhombic loop pairs on the same side of the substrate. Merging orthogonally oriented rhombic loop pairs results in a single‐layer wide stopband FSS with linear reflection phase under normal incidence. Both polarization dependent merged DRL (MDRL) and independent BTB DRL FSSs are developed and experimentally validated. As per measurements, the BTB printed FSS array exhibits 4.3 GHz wide stopband with transmission nulls at 7.9 and 10 GHz while the single side printed FSS exhibits 3.7 GHz wide stopband with transmission null at 8.3 GHz.
“…These characteristics are also obtained by fractal FSSs, 20 combinations of other forms of unit cells, 21,22 and array of rotational symmetric square split ring resonators 23,24 . The band stop FSSs with linear reflection phase behave as good reflectors and thus, these have been assembled with planar antennas to enhance their gain 2,13 …”
Section: Introductionmentioning
confidence: 99%
“…FSSs are two‐ or three‐dimensional structures composed of large array of unit cells arranged in periodic or quasiperiodic fashion to exhibit these characteristics for a desired frequency, multiple frequencies when illuminated by the EM waves 1 . The band stop or band pass filtering characteristics of FSSs have been explored for various applications such as artificial magnetic conductors (AMCs), 2,3 reflectors, 4 absorbers, 5 radomes, 6 and EM shields 7,8 and so forth. Based on symmetry of unit cells toward incident EM waves, the FSSs can either be polarization dependent or independent.…”
Dual rhombic loop (DRL) based low‐cost X‐band frequency selective surfaces (FSSs) with stopband characteristics are presented in this study. Orthogonally oriented arrays of rhombic loop pairs are printed back‐to‐back (BTB) on both sides of dielectric substrate to achieve wide stopband characteristics with stable response under oblique incidences. The nonlinearities in the reflection phase of BTB DRL printed FSSs are compensated by printing orthogonally oriented rhombic loop pairs on the same side of the substrate. Merging orthogonally oriented rhombic loop pairs results in a single‐layer wide stopband FSS with linear reflection phase under normal incidence. Both polarization dependent merged DRL (MDRL) and independent BTB DRL FSSs are developed and experimentally validated. As per measurements, the BTB printed FSS array exhibits 4.3 GHz wide stopband with transmission nulls at 7.9 and 10 GHz while the single side printed FSS exhibits 3.7 GHz wide stopband with transmission null at 8.3 GHz.
“…S- and C-shaped metallic rings are put inside the AMC unit cell to reduce back lobe emission from the patch antenna (Behera et al 2021 ). (Jamali Arand & Abbasi Arand 2021 ) investigated antenna behaviour near-ideal electric, magnetic, and artificial magnetic conductors. The antenna performance has been increased by adjusting the AMC reflection function and the distance between the grounded plane.…”
An artificial magnetic conductor (AMC)-based patch antenna with a low profile is developed for wireless devices in IoT-based healthcare systems. The proposed antenna comprises two pairs of circular-shaped patches with circular-shaped slots and a dual-band 4 × 4 array of AMC reflectors with two zero-degree reflection responses to enhance the antenna's radiation performance. For the 2.45 GHz ISM and 5.4 GHz WLAN bands, the patch antenna has dimensions of 0.44
λ
0
× 0.52
λ
0
× 0.013
λ
0
, with partial ground structures to improve radiation characteristics. Following that, a unique dual-band symmetrical AMC unit cell with dimensions of 22 × 22 × 1.6 mm
3
is developed. There is a gap of 15 mm between the antenna and the AMC surface. The antenna is supported by a 4 × 4 AMC array that has a total dimension of 0.72
λ
0
× 0.72
λ
0
× 0.15
λ
0
. The reflection coefficient values of less than − 10 dB in the 1.7–2.5 and 5.1–5.6 GHz bands, with a bandwidth percentage of 38 and 9.3%, respectively. The antenna's gains were 7.2 and 4 dBi inside the bands. Furthermore, the Specific Absorption Rate (SAR) value did not match the WHO's safety and health guidelines. The issue was solved by including an AMC surface in the proposed antenna. At 2.45 and 5.4 GHz, SAR values of 0.58 and 1.04 W/Kg were measured. Vector network analyser and anechoic chamber were used to test the performance of antenna and AMC surface prototypes. There is a substantial agreement among measured and simulated parameters of an antenna. Consequently, the developed antenna combination with the AMC structure is suited for wireless devices in ISM and WLAN bands, often used in IoT-based healthcare systems.
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