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Application of Defect Induced Microwave Band Gap Structure for Non-destructive Evaluation and the Construction of a FrequencySelector Switch

机译:缺陷诱导微波带隙结构的应用,进行非破坏性评价和频率耦合开关的构造

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The use of microwave band gap structures for the non-destructive evaluation of material property is being probed in this paper. As a first step, we studied numerically, the appearance of a point defect mode within the band gap of a microwave band gap structure for the use as a tool to evaluate the dielectric constant of the material at the defect site. The simulations were carried out using the FEMLAB software. In a pure 10 × 10 square lattice constructed with a material of dielectric constant (ε) 5.5 (in the form of a right circular cylinder), a point defect is created by replacing one of the rods with a geometrically similar but with different dielectric constant material. The appearance of the defect mode is governed by the refractive index contrast (denned as the ratio between the refractive index of the material at the defect site (n_d) and the material of the lattice (n_l). In this case, the refractive index contrast (n_d/n_l) was found to be between 0.85 and 1.28. Simulations were also done with the lattice material of dielectric constant 10 and the defect mode appeared for 1.18 < n_d/n_l < 0.84. For the contrast less than 1, defect creates the fundamental mode similar to TE_(01) mode whereas for the contrast greater than 1, next higher mode similar to TE_(11) appears. Once a defect mode appears, it moves towards lower frequency as the dielectric constant of the defect site is increased. In this paper, we propose to evaluate the dielectric constant of a material using the above procedure. This paper also proposes the construction of a novel frequency selector switch that has two line defects in a 10 × 20 square lattice structure constructed with material of dielectric constant 10.
机译:本文探讨了用于非破坏性评价的微波带隙结构。作为第一步,我们在数值上进行了研究,在微波带隙结构的带隙内的点缺陷模式的外观用作评估缺陷部位的材料的介电常数。使用FEMLAB软件进行模拟。在具有介电常数(ε)5.5的材料构造的纯10×10平方晶格中(以右圆筒的形式),通过用几何上相似但具有不同介电常数的棒来产生点缺陷材料。缺陷模式的外观由折射率对比度(作为缺陷部位(N_D)的材料(N_D)的折射率与晶格(N_L)的材料的比率的比率控制。在这种情况下,折射率对比度(N_D / N_L)被发现为0.85和1.28。也用介电常数10的晶格材料进行仿真,缺陷模式出现为1.18

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