## Abstract A convex hexahedral TLM mesh of arbitrary shape is presented and the transmission‐line matrix method extended to any non‐orthogonal configuration. The novel mesh constitutes a natural generalization of Johns' condensed node. The associated TLM process is analysed and reconstructed as a
Consistent finite difference modelling of Maxwell's equations with lossy symmetrical condensed TLM node
✍ Scribed by Steffen Hein
- Publisher
- John Wiley and Sons
- Year
- 1993
- Tongue
- English
- Weight
- 637 KB
- Volume
- 6
- Category
- Article
- ISSN
- 0894-3370
No coin nor oath required. For personal study only.
✦ Synopsis
A propagator integral interpretation for general TLM processes is presented and applied to discretized Maxwell's equations. The approach provides exact algebraic solutions of finite difference equations along a quite universal scheme.
Specifically, Johns's process based on the symmetrical condensed node is reconstructed and generalized as a clear-cut FD algorithm. The fields computed are exact time-domain solutions of the FD equations, provided that total voltages and currents are evaluated and stub quantities are not externally excited. Losses are very naturally incorporated into the TLM algorithm.
The structural similarity of the TLM process (properly operated) with the propagator integral appears just as fundamental as general and should have further applications.
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