Figure 7 Measured S-parameters of the microstrip passive dualbeam scanning leaky-wave antenna two-feed topology for the active leaky-wave antenna in order to create a dual-beam radiation pattern, and vary the frequency of the HEMT VCO to control a two-directional scanning beam. The total measured sc
A hybrid TLM-FDTD method for the modelling of diffusion
โ Scribed by Chi Chung Wong; Cynthia Lee
- Publisher
- John Wiley and Sons
- Year
- 2000
- Tongue
- English
- Weight
- 120 KB
- Volume
- 13
- Category
- Article
- ISSN
- 0894-3370
No coin nor oath required. For personal study only.
โฆ Synopsis
A new hybrid TLM-FDTD algorithm for solving di!usion problems is described. The method utilizes the transmission line model to de"ne the time step and the FDTD's leap-frog algorithm to determine the voltages and currents of the network analogue of the di!usion equation. Unlike the standard TLM method, the proposed one does not generate spurious oscillations. The method is explicit and can be used to solve highly non-linear problems without the need to solve non-linear equations. The implementation of a simple adaptive time-stepping algorithm is also described.
๐ SIMILAR VOLUMES
We show that the general boundary condition DaWax + a@ = 0 (D is the diffusion coefficient and a is a ## constant) in TLM diffusion modelling can be expressed accurately in terms of a voltage reflection coefficient p = ( A x -a A t ) / ( A x + aAt), where Ax is the spatial resolution and At is the
There is a class of material processing simulators which require solution of the diffusion equation over a surface which is evolving due to some physical or chemical process related to the concentration of the diffusing species. Because of its explicit and unconditionally stable nature, the transmis
The suitability of the transmission line modelling method for studying field-particle interaction devices is assessed through an example of a simple two-cavity klystron amplifier. Two separate numerical studies are presented, covering both beam bunching in the buncher cavity and field generation in
Figure 4 Directive gain plot for the full 27 = 27 planar array. Spacing between the elements in the array is held constant at d s r2 with s 0ะ. The maximum directive gain for this array is D s 30.46 dB belong to the family of Sierpinski carpets. An example was considered in which sum and difference