Abstract
In contrast to the TLM scheme for the symmetrical condensed node (SCN), the field variables of the alternating transmission line matrix scheme (ATLM) are sampled at the center of the three-dimensional TLM cell. Considering the spatial derivatives of the electric and magnetic field components yields a bijective one-to-one mapping between the six field components, six spatial derivatives of the field components and the twelve wave amplitudes. ATLM does not support any nonphysical or spurious solutions and it represents the only TLM scheme with the same number of linearly independent field variables per cell as Yee's FDTD scheme.
| Original language | English |
|---|---|
| Pages | 238-245 |
| Number of pages | 8 |
| State | Published - 1996 |
| Externally published | Yes |
| Event | Proceedings of the 1996 12th Annual Review of Progress in Applied Computational Electromagnetics. Part 1 (of 2) - Monterey, CA, USA Duration: 18 Mar 1996 → 22 Mar 1996 |
Conference
| Conference | Proceedings of the 1996 12th Annual Review of Progress in Applied Computational Electromagnetics. Part 1 (of 2) |
|---|---|
| City | Monterey, CA, USA |
| Period | 18/03/96 → 22/03/96 |