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Coupling analysis of isotropic and anisotropic dielectric materials in rectangular waveguide
Hidayat M.R.a, Munir A.a
a Radio Telecommunication and Microwave Laboratory, School of Electrical Engineering and Informatics, Institut Teknologi Bandung, Indonesia
[vc_row][vc_column][vc_row_inner][vc_column_inner][vc_separator css=”.vc_custom_1624529070653{padding-top: 30px !important;padding-bottom: 30px !important;}”][/vc_column_inner][/vc_row_inner][vc_row_inner layout=”boxed”][vc_column_inner width=”3/4″ css=”.vc_custom_1624695412187{border-right-width: 1px !important;border-right-color: #dddddd !important;border-right-style: solid !important;border-radius: 1px !important;}”][vc_empty_space][megatron_heading title=”Abstract” size=”size-sm” text_align=”text-left”][vc_column_text]© 2016 IEEE.In this paper, the coupling analysis of two loaded resonators inside of a TE mode rectangular waveguide is investigated. The resonators are made of isotropic and anisotropic dielectric materials which have specific parameters of relative permittivity and thickness as a function of separation between resonators. Each resonator is composed of conventional and modified dielectric materials which are divided into three parts in specific percentages. The analysis is carried out by calculating theoretically the coupling coefficient from each corresponding resonant frequency for different parameter. Then the theoretical calculations of coupling coefficient for each parameter are compared to the results of parametric study obtained from simulation. From the results, it shows that the coupling coefficient for isotropic and anisotropic dielectric materials in a rectangular waveguide are similar each other when the values of relative permittivity, ϵr and ϵy, are 12 for isotropic and anisotropic dielectric materials, respectively.[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Author keywords” size=”size-sm” text_align=”text-left”][vc_column_text]Anisotropic,Anisotropic dielectrics,Coupling coefficient,isotropic,Loaded resonators,Relative permittivity,Resonance frequencies,Theoretical calculations[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Indexed keywords” size=”size-sm” text_align=”text-left”][vc_column_text]Anisotropic,coupling coefficient,isotropic,rectangular waveguide,resonance frequency[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Funding details” size=”size-sm” text_align=”text-left”][vc_column_text][/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”DOI” size=”size-sm” text_align=”text-left”][vc_column_text]https://doi.org/10.1109/ICITACEE.2016.7892488[/vc_column_text][/vc_column_inner][vc_column_inner width=”1/4″][vc_column_text]Widget Plumx[/vc_column_text][/vc_column_inner][/vc_row_inner][/vc_column][/vc_row][vc_row][vc_column][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][/vc_column][/vc_row]