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Series Combination of One-Ports

Figure J.6 shows the series combination of two one-ports.

Figure J.6: Two one-port networks combined in series. The impedance of the series combination is $ R(s) = F(s)/V(s) = R_1(s) + R_2(s)$.
\includegraphics[scale=0.9]{eps/lseries}

Impedances add in series, so the aggregate impedance is $ R(s) = R_1(s) + R_2(s)$, and the admittance is

$\displaystyle \Gamma(s) = \frac{1}{\frac{1}{\Gamma_1(s)} + \frac{1}{\Gamma_2(s)}} =
\frac{\Gamma_1(s) \Gamma_2(s) }{\Gamma_1(s) + \Gamma_2(s)}
$

The latter expression is the handy product-over-sum rule for combining admittances in series.

In a physical situation, if two elements are connected in such a way that they share a common velocity, then they are in series. An example is a mass connected to one end of a spring where the other end is attached to a rigid support and the force is applied to the mass, as shown in Fig. J.7.

Figure J.7: A mass and spring combined as one-ports in series.
\includegraphics[scale=0.9]{eps/lseriesExample}


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[How to cite and copy this work] 
``Physical Audio Signal Processing for Virtual Musical Instruments and Digital Audio Effects'', by Julius O. Smith III, (December 2005 Edition).
Copyright © 2006-07-01 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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