This paper presents a proof of convergence of the transmission-line matrix
(TLM) method with a symmetrical condensed node (SCN) in the classical formu
lation of Johns. It is shown that the convergence order of the SCN-TLM meth
od cannot simply be derived from observing the dispersion characteristics o
f the TLM mesh, The mapping between the discretized electromagnetic field a
nd TLM wave amplitudes plays a decisive role. Although second-order converg
ence is observed for coarse discretizations, which are usually used in prac
tice due to the limitations of memory resources, it is shown and numericall
y verified that the asymptotic convergence reduces to order O(root Deltat).
Only using a bijective field mapping defined at the cell boundaries yields
second-order convergence.