2014
DOI: 10.1063/1.4902855
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A Cantor multilayer traveling wave applicator for microwave heating: Numerical analysis and design

Abstract: A traveling wave applicator particularly suitable for heating low loss materials is described. The applicator consists of a dielectric Cantor multilayer inserted in a single-mode rectangular metallic waveguide. Field localization phenomenon occurring in the multilayer allows high field amplitude (several times the amplitude of the incident field) to be obtained in a load placed at the center of the applicator. Design examples and numerical characterization of an applicator in WR-284 waveguide operating at 2.45… Show more

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Cited by 9 publications
(11 citation statements)
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“…This fractal construction consists of an initiator (which is the structure at the zeroth stage of growth) and a procedure generating the structure at the stage of growth M+1 from the one at the stage of growth M. In our case the initiator is a dielectric layer with relative permittivity d and thickness L while the generating procedure consists in removing the middle Rth part (R >1) of the dielectric layers at the stage of growth M leaving air gaps in their places ( a = 1). In this paper resonators at the stage of growth M = 2 will be considered, because they seem to offer a good trade-off between structure complexity and field localization property [Chiadini et al, 2008b[Chiadini et al, , 2014. As shown in Figure 1, at the stage M = 2 the Cantor resonator has a very simple structure consisting of four equal thickness dielectric layers separated by three air gaps with different lengths.…”
Section: Cantor Dielectric Resonatormentioning
confidence: 99%
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“…This fractal construction consists of an initiator (which is the structure at the zeroth stage of growth) and a procedure generating the structure at the stage of growth M+1 from the one at the stage of growth M. In our case the initiator is a dielectric layer with relative permittivity d and thickness L while the generating procedure consists in removing the middle Rth part (R >1) of the dielectric layers at the stage of growth M leaving air gaps in their places ( a = 1). In this paper resonators at the stage of growth M = 2 will be considered, because they seem to offer a good trade-off between structure complexity and field localization property [Chiadini et al, 2008b[Chiadini et al, , 2014. As shown in Figure 1, at the stage M = 2 the Cantor resonator has a very simple structure consisting of four equal thickness dielectric layers separated by three air gaps with different lengths.…”
Section: Cantor Dielectric Resonatormentioning
confidence: 99%
“…Equations (1)-(3) indicate that the geometry of the resonator is unambiguously determined fixing two of the three parameters D, L, and R. When inserted in metallic rectangular waveguide, a Cantor resonator exhibits a transmissivity spectrum with forbidden bands and narrow transmission peaks in the single-mode frequency range of the waveguide [Chiadini et al, 2009]. At the frequencies corresponding to the peaks a resonance phenomenon occurs, yielding energy concentration and field localization in the central air gap [Chiadini et al, 2014].…”
Section: Cantor Dielectric Resonatormentioning
confidence: 99%
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“…HF wave thermal treatment pays an important role in producing heat-insulating building materials due to high inefficiency of the existing convection heating methods which is responsible for the low coefficient of thermal conductivity of heat-insulating materials [5].…”
Section: Introductionmentioning
confidence: 99%