Abstract:Introducing a thin conductive layer into a finite-mesh (as inherent in e.g. finite difference time domain (FDTD) and finite element (FEM) methods) typically requires a dedicated equivalent macroscopic model allowing for computationally effective and accurate electromagnetic (EM) and thermal simulations. Thin conductive layers, such as microwave susceptors, characterised by their surface resistance (Rs), are adequately represented with a dielectric surrogate layer of higher thickness and proportionally scaled c… Show more
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