## Abstract In Part I, two TLM‐based solutions were presented for the Klein–Gordon Equation in its basic form, with the TLM pulses representing the primary variable. In Part II, two further approaches are presented in which the TLM pulses now represent derivatives of the primary variable, with resp
TLM-based solutions of the Klein–Gordon equation (Part I)
✍ Scribed by William J. O'Connor; Fergus J. Clune
- Publisher
- John Wiley and Sons
- Year
- 2001
- Tongue
- English
- Weight
- 123 KB
- Volume
- 14
- Category
- Article
- ISSN
- 0894-3370
- DOI
- 10.1002/jnm.425
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✦ Synopsis
Abstract
The transmission line matrix (TLM) method has become well established as a numerical solution scheme for wave problems in electromagnetics and, to a lesser extent, in acoustics and mechanics. It has also been applied to diffusion/heat‐conduction problems. Here the technique is extended to solving the Klein–Gordon equation that arises in Quantum Mechanics and in the dynamics of an elastically anchored vibrating string. In Part I, two novel, TLM‐based algorithms are presented and verified. By considering them as solving a special case of the more general ‘forced’ wave equation, they illustrate how, with care, the TLM algorithm can be adapted to model a wide range of effects. Copyright © 2001 John Wiley & Sons, Ltd.
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