## Abstract The analysis of lossy nonreciprocal transmission line (LNTL in short), which is the most general case in transmission line problems, is presented in this article. By modifying the expression of input impedance, we get a novel graphical tool called omnipotent Smith chart (OSC) for solvin
An extended omnipotent Smith chart with active parameters
✍ Scribed by Yongle Wu; Haiyu Huang; Yuanan Liu
- Book ID
- 102522797
- Publisher
- John Wiley and Sons
- Year
- 2008
- Tongue
- English
- Weight
- 182 KB
- Volume
- 50
- Category
- Article
- ISSN
- 0895-2477
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✦ Synopsis
Abstract
The lossy nonreciprocal transmission line (LNTL) model with active characteristic impedances and active load impedances is researched in this article. For solving LNTL problems involving active parameters, the previous presented omnipotent Smith chart (OSC) is extended its domain of application. Though the formation of expression is unchanged, the extended OSC (EOSC) shows different characteristics. The EOSC is especially significant for the application in oscillator design and amplifier stabilization. An EOSC can be easily generated using Matlab or Java for applications. © 2008 Wiley Periodicals, Inc. Microwave Opt Technol Lett 50: 896–899, 2008; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.23229
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## Abstract Originally published in Microwave Opt Technol Lett 49: 2392–2395, 2007. © 2007 Wiley Periodicals, Inc. Microwave Opt Technol Lett 50: 263, 2008; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mop.23053
## Abstract It has been shown recently in the literature that the conjugately characteristic‐impedance transmission lines (CCITLs) implemented by periodically loaded lossless lines can exhibit active characteristic impedances (i.e., negative characteristic resistances). In this case, the magnitude
## Abstract Conjugately characteristic‐impedance transmission lines (CCITLs) implemented by lossless periodic transmission‐line structures can exhibit active characteristic impedances; that is, negative characteristic resistances. In this case, the magnitude of the voltage reflection coefficient is