Proceedings of the 30th International on Design Automation Conference - DAC '93 1993
DOI: 10.1145/157485.165108
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S-parameter based macro model of distributed-lumped networks using exponentially decayed polynomial function

Abstract: A Scattering-Parameters {S-Parameters) based macromodel of distributed-lumped networks is presented. The networb can include capacitive cutsets, inductive loops, RLC meshes, and lossy transmission lines. An ef)cienl network reduction algorithm is &veloped to reduce [he original nelwork into a network containing one multipor[ component together with the sources and loads of interest. The S-Parameters of the circuit components are approximated by Taylor series to simpllfi the reduction process. Exponentially Dec… Show more

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Cited by 24 publications
(7 citation statements)
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“…positive poles for Pade approximation [14], but usually arises in fitting the attenuation data of frequency-dependent lines.…”
Section: However Ifmentioning
confidence: 99%
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“…positive poles for Pade approximation [14], but usually arises in fitting the attenuation data of frequency-dependent lines.…”
Section: However Ifmentioning
confidence: 99%
“…In order to simplify the following discussion, consider the well known trapezoidal rule for numerical integration. In other words, approximate the "excitation" as (14) where , , and is the remainder term. Substitution of (14) into (13) and performing the integration yields (15) where and Note that is the error due to the interpolation for .…”
Section: However Ifmentioning
confidence: 99%
“…In the second category, the moment-matching technique has been used to approximate waveforms of a linear interconnect network using its lower order moments [6,7,8]. Since the advent of Asymptotic Waveform Evaluation(AWE) technique, many interconnect delay evaluation models [9,10,11] have been proposed.…”
Section: Introductionmentioning
confidence: 99%
“…The basic electrical parameters of a transmission line are resistance along the line, inductance along the line, conductance shunting the line, and capacitance shunting the line. (1) (2) By combining equations (1) and (2), we can come up with the following equation: (3) Equations (1), (2), (3) are the fundamental relationships governing wave propagation along a uniform transmission line. The shunt conductance is often negligible, hence we set g=0.…”
Section: Introductionmentioning
confidence: 99%