1994
DOI: 10.1109/22.310590
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Analysis of packaged microwave integrated circuits by FDTD

Abstract: The behavior of packaged single and coupled MMIC via-hole grounds has been investigated by using a graded mesh FDTD code running on the massive parallel computer DEC 12000 with 4 K processors. Theoretical simulations have been compared with experimental measurements showing excellent agreement.Moreover, since the package introduces resonances, we have also investigated several different possibilities to choke off these resonances. It is shown that the common practice of inserting a damping layer just below the… Show more

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Cited by 27 publications
(5 citation statements)
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References 32 publications
(6 reference statements)
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“…This way, for the case of conductors of finite extent, homogeneous-medium Green's functions are used in the integral representations of the potentials, as shown in the equations above. With these assumptions, inserting (2) and (3) into (1), and enforcing (1) at a point inside one of the conductors, we obtain an expression involving the unknown quantities and as follows: (4) where is the conductivity at the specific point inside the conductor. In order to solve the system of equations in (4), the current and charge densities are discretized into volume and surface cells, respectively.…”
Section: Development Of Peec Modelsmentioning
confidence: 99%
“…This way, for the case of conductors of finite extent, homogeneous-medium Green's functions are used in the integral representations of the potentials, as shown in the equations above. With these assumptions, inserting (2) and (3) into (1), and enforcing (1) at a point inside one of the conductors, we obtain an expression involving the unknown quantities and as follows: (4) where is the conductivity at the specific point inside the conductor. In order to solve the system of equations in (4), the current and charge densities are discretized into volume and surface cells, respectively.…”
Section: Development Of Peec Modelsmentioning
confidence: 99%
“…Let the transmission lines in Figure 1 have identical characteristics, and let Ff, be the reflection coefficient at the far-end wall and the propagation constant, respectively, corresponding to the dominant propagating mode. The source boundary reflection is minimized by using a matched source, wherein the circuit is excited in the source plane by a quasistatically computed transverse field distribution [20], and the source plane is replaced by Mur's ABC after the source waveform is established. Hence, the reflection from source-end boundary is not considered in the analysis.…”
Section: Discontinuity Characterizationmentioning
confidence: 99%
“…Possible solutions are to use the same perimeter, equal area, or simply taking the diameter as side length of the square. Although probably everyone involved in em simulations came across this problem once and via modeling has been treated in the literature quite frequently (see, e.g., [5][6][7][8][9]), nothing appears to have been published on this small but useful detail. This is presented in the following.…”
Section: Introductionmentioning
confidence: 99%