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Physical Interpretation of Reflection and Transmission in Lumped Systems

In lumped systems, traveling waves do not occur, in principle, because lumped elements are characterized as one-ports interconnected by ``wires'' having no time delay associated with them. It may therefore seem strange that a scattering theory formulation exists for lumped networks.

There does exist, however, a physical interpretation of reflection and transmission in lumped networks [34]. Suppose we have a ``force source'' $ f(t)$ which drives a ``load impedance'' $ R_1$ in series with a ``source impedance'' $ R_0$. For simplicity, let the load and source impedances be real (dashpots) as shown in Fig. L.20.

Figure L.20: A series connection of two dashpots $ R_0$ and $ R_1$ driven by a force $ f(t)$. Dashpot $ R_0$ models the source impedance, while $ R_1$ models a load impedance.
\includegraphics[width=3in]{eps/lparallel_dashpots}
An equivalent electrical circuit is shown in Fig. L.21.

Figure L.21: Equivalent circuit of a dashpot $ R_1$ driven by a force source $ f(t)$ with internal impedance $ R_0$.