References
- Pulko , S. H. , Mallik , A. and Johns , P. B. 1986 . Application of Transmission Line Modelling to Thermal Diffusion in Bodies of Complex Geometry, Int . J. Numer. Meth. Eng. , 23 : 2303 – 2312 .
- deCogan , D. and John , S. A. 1985 . Failure Modes in Punch Through Diodes, J . Phys. D: Appl. Phys. , 18 : 497 – 505 .
- Hurst , A. I. and Pulko , S. H. 1994 . TLM Treatments of Changes of Phase . Int. J. Munter. Mod. , 7 : 201 – 207 .
- S. H. Pulko, H. R. Newton, A. I. Hurst, J. M. Gilbert, and A J. Wilkinson, Combined Heat Transfer and Deformation Modelling for Ceramics Firing, IEE Comput. and Control J., February 1999.
- deCogan , D. and Soulos , A. 1996 . Inverse Thermal Modelling Using TLM, Numer . Heat Transfer B , 29 : 125 – 135 .
- D. deCogan, A. Soulos, and K. O. Chichlowski, Sub-surface Feature Location and Identification Using Inverse TLM Techniques. Microelertran. J. vol. 29. pp. 215-222, 1998.
- W. J. R. Hoefer and M. Forest, TLM Modelling of Electromagnetic Scattering in Forward and Reverse Time Sequence. Proc. ISAP '92. Sapporo. Japan, pp. 733-736.
- M. Forest and W. J. R. Hoefer, A Novel Synthesis Technique for Conducting Scatterers Using the TLM Technique. IEEE Trans. Microwave Theory Tech.. vol. 43, pp. 1371-1378, 1995.
- D. deCogan, Transmission Line Matrix (TLM) Techniques for Diffusion Applications, Gordon & Breach, 1998.
- S. H. Pulko, A. J. Wilkinson, and A. Saidane, TLM Representation of the Hyperbolic Heat Conduction Equation. Int. J. Numer. Mod., in press.
- Gilbert , J. M. , Wilkinson , A. J. and Pulko , S. H. 2000 . The Effect of Stubs on the Dynamics of TLM Diffusion Modelling Networks, Numer . Heat Transfer B , 37 : 165 – 184 .
- Johns , P. B. and Butler , G. 1983 . The Consistency and Accuracy of the TLM Method for Diffusion and Its Relationship to Existing Techniques . Int. J. Numer. Meth. Eng. , 19 : 1949 – 1954 .
- Enders , P. and deCogan , D. 1996 . Discrete Models of Heatflow in Multilayer Materials Using Simple and Correlated Random Walks, Int . J. Numer. Mod. , 9 : 445 – 457 .