An unconditionally stable precise integration time-domain method is extended to 3-D circular cylindrical coordinates to solve Maxwell's equations. In contrast with the cylindrical finite-difference time-domain method, not only can it remove the stability condition restraint, but also make the numeri
A Crank–Nicholson-based unconditionally stable time-domain algorithm for 2D and 3D problems
✍ Scribed by Xin Xie; George Pan; Stephen Hall
- Publisher
- John Wiley and Sons
- Year
- 2006
- Tongue
- English
- Weight
- 221 KB
- Volume
- 49
- Category
- Article
- ISSN
- 0895-2477
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✦ Synopsis
Abstract
It has been shown that both ADI‐FDTD and CN‐FDTD are unconditionally stable. While the ADI is a second‐order approximation, CN is only in the first order. However, analytical expressions reveal that the CN‐FDTD has much smaller truncation errors and is more accurate than the ADI‐FDTD. Nonetheless, it is more difficult to implement the CN than the ADI, especially for 3D problems. In this paper, we present an unconditionally stable time‐domain method, CNRG‐TD, which is based upon the Crank–Nicholson scheme and implemented with the Ritz–Galerkin procedure. We provide a physically meaningful stability proof, without resorting to tedious symbolic derivations. Numerical examples of the new method demonstrate high precision and high efficiency. In a 2D capacitance problem, we have enlarged the time step, Δt, 400 times of the CFL limit, yet preserved good accuracy. In the 3D antenna case, we use the time step, Δt, 7.6 times larger that that of the ADI‐FDTD i.e., more than 38 times of the CFL limit, with excellent agreement of the benchmark solution. © 2006 Wiley Periodicals, Inc. Microwave Opt Technol Lett 49: 261–265, 2007; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.22101
📜 SIMILAR VOLUMES
This paper presents a 3D body-conforming "nite element solution of the time-dependent vector wave equation. The method uses edge elements on tetrahedra for the electric "eld interpolation. This kind of element is suited to model Maxwell's equations since it only enforces tangential continuity of vec