Analysis and design of substrate integrated waveguide using efficient 2d hybrid method wu xuan hui kishk ahmed
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Finally, a practical microstrip balanced-to-unbalanced power divider, which operates at 0. The scattering matrices of all the building blocks are cascaded and the scattering matrix of the whole filter is obtained. Moreover, the inter-digital coplanar stripline used in the step-impedance section effectively reduces the characteristic impedance of the transmission line for large size shrinkage and insertion-loss reduction. Recently, a new type of transmission line called substrate integrated waveguide or post-wall waveguide is invented. Finally, a practical microstrip balanced-to-unbalanced power divider, which operates at 0. Near the antenna, the field is elliptically polarized.

Volume 4A, 3-8 July 2005 Page s : 321 â 324 Vol. It combines the cylindrical eigenfunction expansion and the method of moments to avoid geometrical descritization of the posts. First, a closed contour is generated to enclose the circuit as shown in Fig. For the ease of the design of implanted low-profile antennas, simplified planar geometries based on a real human body are proposed. The near field of uninsulated dipole antenna in a dissipative dielectric medium is important in microwave hyperthermia and geophysical applications. But, thin wire approximation that assumes a uniform circumferential current density may be invalid for a metal post on the post wall even if it is electrically thin because the current density on the post wall looking from inside of the circuit is much stronger than that looking from outside of the circuit.

Its S parameters are obtained and validated in Fig. The gray cylinder, referred to source cylinder q, scatters field, while the cylinder in dashed line, referred to observation cylinder p, is the one where the boundary conditions are applied. Furthermore, the study demonstrates that by distributing the transmitted power over several frequency bands, more accurate estimation can be achieved due to frequency diversity, and the negative effects of radiation pattern deviation can be alleviated. For a network with n sub-ports as shown in Fig. If the observation point x, y is not located on the magnetic current itself, 4.

He received the Microwave Theory and Techniques Society Microwave Prize 2004. The radiation performances of the designed low-profile antennas are estimated in terms of radiation patterns, radiation efficiency, and specific absorption rate. The phase shifter dimensions are 4 Ã 4. Thereafter, we would expand the scattered field on both sides of the grating in Floquet modes and apply accurate boundary conditions such that the tangential E-field is zero at the surface of each strip and continuous between the strips. For the problem in Fig. First, the electromagnetic field expressions in the substrate are obtained. Considering linear devices only where the superposition principle holds, as the superposition of the excitations in Fig.

The field inside the waveguide is expressed in terms of cylindrical vector wave-functions and the finite conductivity of the top and of the bottom plates, and of the metallic vias are taken into account. It acts as a bandpass filter that allows the electromagnetic waves between 27. The external rectangular waveguide allows to easily segment the structure into building blocks that are composed of circular metallic vias inside a rectangular waveguide. It inherits the merits both from the microstrip for compact size and easy integration, and from the waveguide for low radiation loss, and thus opens another door to design efficient microwave circuits and antennas at a low cost. Since 2009, he is with Radio Waves Inc. Then, as an application, an in-line dual-mode rectangular waveguide bandpass filter is analyzed using the proposed method along with generalized scattering matrix method. Consequently, the vertical current flows on the through holes and the longitudinal current flows along the middle strips to meet the wave propagation requirement in the E-plane waveguide circuit.

Coaxial ports are considered as sources and self and mutual admittances are evaluated. It can be found that the upper side response of the circular cavity and the lower side response of the elliptic cavity are very steep. In addition, a procedure for accurately designing tapered microstrip-to-substrate integrated waveguide transitions is described. The problem is considered as a 2-D electromagnetic problem assuming no field variation normal to the dielectric substrate. Microwave Theory and Techniques, vol. The S-parameters of the post-wall circuits, which act as bandpass filters, are calculated using the image theory combined with the lattice sums technique. In this paper, a derived theoretical model shows that, for certain values for the odd- and even-mode impedances, a coupled structure with a length that is less than one tenth of a wavelength is sufficient to build a high-performance reflection phase shifter.

A filter design method derived from a synthesis technique using inductive post is presented. This idea can be applied to halve a circuit size while keeping its electrical characteristics. Whole-body software models homogeneous, layered and tissue-segmented were developed for an adult male subject. The simulated results are plotted in Fig. Due to the maturity of the planar fabrication technique, an array of either the slot antennas or sectoral horn antennas can be fabricated together with the feeding network on a single printed circuit board. Similar to a circuit with only metallic posts as discussed in Chapter 2, the equation 3.

The computed results are compared with those previously obtained by an approximate numerical calculation. The theoretical results are compared with measurements performed on prototypes and good agreement Is obtained. The antenna is optimized for dual-band operation by combining an in-house finite-element boundary integral electromagnetic simulation code and particle swarm optimization algorithm. Strictly speaking, the problem in Fig. The input and of the prototype with a relative phase shifting of 292.