### Abstract

In modeling wave propagation using the Finite Difference Time Domain (FDTD) method, the field gradients at each point are calculated using central difference approximation. For points on the edge of the model volume a separate algorithm to simulate absorbing boundaries has to be used. Most of these absorbing boundary conditions assume normal wave incidence at the boundary, but at the sides of stripline or microstrip this is not the case. This letter proposes a variant of dispersive boundary conditions with one phase velocity given an infinite value to represent a wave travelling parallel to the boundary. When applied to uniform stripline, these boundary conditions gave better results than the original version of the dispersive boundary condition with two finite phase velocities. These boundary conditions enable the use of a smaller calculation volume, thus saving computing memory and time.

Original language | English |
---|---|

Pages (from-to) | 241-242 |

Number of pages | 2 |

Journal | IEEE Microwave and Guided Wave Letters |

Volume | 5 |

Issue number | 8 |

DOIs | |

Publication status | Published - 1 Aug 1995 |

### ASJC Scopus subject areas

- Engineering(all)
- Physics and Astronomy(all)

### Cite this

*IEEE Microwave and Guided Wave Letters*,

*5*(8), 241-242. https://doi.org/10.1109/75.401080

**Absorbing Boundary Conditions for the Modeling of Scatterers in Parallel-Plate Transmission Media.** / Spillard, C.; Pennock, S. R.; Shepherd, P. R.

Research output: Contribution to journal › Article

*IEEE Microwave and Guided Wave Letters*, vol. 5, no. 8, pp. 241-242. https://doi.org/10.1109/75.401080

}

TY - JOUR

T1 - Absorbing Boundary Conditions for the Modeling of Scatterers in Parallel-Plate Transmission Media

AU - Spillard, C.

AU - Pennock, S. R.

AU - Shepherd, P. R.

PY - 1995/8/1

Y1 - 1995/8/1

N2 - In modeling wave propagation using the Finite Difference Time Domain (FDTD) method, the field gradients at each point are calculated using central difference approximation. For points on the edge of the model volume a separate algorithm to simulate absorbing boundaries has to be used. Most of these absorbing boundary conditions assume normal wave incidence at the boundary, but at the sides of stripline or microstrip this is not the case. This letter proposes a variant of dispersive boundary conditions with one phase velocity given an infinite value to represent a wave travelling parallel to the boundary. When applied to uniform stripline, these boundary conditions gave better results than the original version of the dispersive boundary condition with two finite phase velocities. These boundary conditions enable the use of a smaller calculation volume, thus saving computing memory and time.

AB - In modeling wave propagation using the Finite Difference Time Domain (FDTD) method, the field gradients at each point are calculated using central difference approximation. For points on the edge of the model volume a separate algorithm to simulate absorbing boundaries has to be used. Most of these absorbing boundary conditions assume normal wave incidence at the boundary, but at the sides of stripline or microstrip this is not the case. This letter proposes a variant of dispersive boundary conditions with one phase velocity given an infinite value to represent a wave travelling parallel to the boundary. When applied to uniform stripline, these boundary conditions gave better results than the original version of the dispersive boundary condition with two finite phase velocities. These boundary conditions enable the use of a smaller calculation volume, thus saving computing memory and time.

UR - http://www.scopus.com/inward/record.url?scp=0029357456&partnerID=8YFLogxK

U2 - 10.1109/75.401080

DO - 10.1109/75.401080

M3 - Article

VL - 5

SP - 241

EP - 242

JO - IEEE Microwave and Guided Wave Letters

JF - IEEE Microwave and Guided Wave Letters

SN - 1051-8207

IS - 8

ER -