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@MastersThesis{Greco:2013:AnMoLi,
               author = "Greco, Ana Fl{\'a}via Guedes",
                title = "An{\'a}lise e modelagem de linhas de transmiss{\~a}o n{\~a}o 
                         lineares com elementos concentrados nas configura{\c{c}}{\~o}es 
                         LC e CL",
               school = "Instituto Nacional de Pesquisas Espaciais (INPE)",
                 year = "2013",
              address = "S{\~a}o Jos{\'e} dos Campos",
                month = "2013-11-27",
             keywords = "linhas de transmiss{\~a}o n{\~a}o lineares, solu{\c{c}}{\~a}o 
                         num{\'e}rica de equa{\c{c}}{\~o}es diferenciais n{\~a}o 
                         lineares, modelagem e simula{\c{c}}{\~a}o, gera{\c{c}}{\~a}o 
                         de RF, gera{\c{c}}{\~a}o de s{\'o}litons claros e escuros, 
                         nonlinear transmission lines, numerical solution of nonlinear 
                         differential equations, modeling and simulation, RF generation by 
                         nonlinear transmission lines, generation of bright and dark 
                         solitons.",
             abstract = "Em uma formula{\c{c}}{\~a}o geral descrita por um sistema de 
                         equa{\c{c}}{\~o}es diferenciais ordin{\'a}rias no 
                         dom{\'{\i}}nio do tempo, o presente trabalho de 
                         disserta{\c{c}}{\~a}o investiga os fen{\^o}menos de 
                         propaga{\c{c}}{\~a}o em linhas de transmiss{\~a}o lineares e 
                         n{\~a}o lineares constitu{\'{\i}}das de c{\'e}lulas LC e CL. 
                         Foram desenvolvidas e em seguida comparadas duas 
                         formula{\c{c}}{\~o}es matem{\'a}ticas, importantes do ponto de 
                         vista conceitual, mas pouco discutidas na literatura. Para a 
                         primeira formula{\c{c}}{\~a}o tem-se como vari{\'a}veis de 
                         estado a corrente de malha que circula em cada se{\c{c}}{\~a}o, 
                         e a correspondente carga armazenada em cada capacitor. Para a 
                         outra formula{\c{c}}{\~a}o consideram-se a corrente no indutor 
                         de cada se{\c{c}}{\~a}o e a tens{\~a}o nos capacitores. De 
                         import{\^a}ncia sob o aspecto num{\'e}rico e uma vez que existem 
                         poucos estudos sobre tais formula{\c{c}}{\~o}es, foram adotadas 
                         estas vari{\'a}veis de maneira que as equa{\c{c}}{\~o}es 
                         diferenciais sejam todas de primeira ordem. A 
                         formula{\c{c}}{\~a}o desenvolvida foi escrita para que a cada 
                         elemento discreto em uma se{\c{c}}{\~a}o particular i possam ser 
                         atribu{\'{\i}}dos valores arbitr{\'a}rios L\$_{i}\$ e 
                         C\$_{i}\$. Al{\'e}m disso, a formula{\c{c}}{\~a}o permite a 
                         an{\'a}lise no regime transit{\'o}rio das linhas sendo excitadas 
                         por um pulso de forma arbitr{\'a}ria. No regime linear, foram 
                         examinadas as caracter{\'{\i}}sticas de propaga{\c{c}}{\~a}o 
                         em linhas peri{\'o}dicas, nas quais c{\'e}lulas unit{\'a}rias 
                         id{\^e}nticas repetem-se periodicamente, e tamb{\'e}m linhas 
                         duplamente peri{\'o}dicas, onde cada se{\c{c}}{\~a}o 
                         {\'{\i}}mpar comp{\~o}e-se de um par de elementos L\$_{1}\$ e 
                         C\$_{1}\$, enquanto as se{\c{c}}{\~o}es pares incluem um 
                         indutor L\$_{2}\$ e um capacitor C\$_{2}\$. Na 
                         atribui{\c{c}}{\~a}o dos valores dos elementos do circuito dois 
                         casos foram considerados. Para linhas peri{\'o}dicas destaca-se a 
                         interpreta{\c{c}}{\~a}o de velocidades de fase positiva e 
                         negativa associadas respectivamente {\`a}s topologias LC e CL, 
                         considerando um sinal senoidal. J{\'a} para linhas duplamente 
                         peri{\'o}dicas destaca-se o car{\'a}ter de filtragem espacial, 
                         uma vez que as linhas assim sintetizadas com elementos 
                         concentrados exibiram forte dispers{\~a}o espacial em que cada 
                         n{\'o} da linha apresenta um espectro distinto de 
                         frequ{\^e}ncia. No regime n{\~a}o linear, foram investigados 
                         alguns fen{\^o}menos associados {\`a} linha LC tais como 
                         gera{\c{c}}{\~a}o de RF, gera{\c{c}}{\~a}o de s{\'o}litons, e 
                         redu{\c{c}}{\~a}o dos tempos de subida e de descida de pulsos 
                         que se propagam ao longo da linha. E para linhas CL foram 
                         investigados a forma{\c{c}}{\~a}o de s{\'o}litons claros e 
                         escuros (que constituem caracter{\'{\i}}sticas {\'u}nicas das 
                         linhas CL) e tamb{\'e}m a gera{\c{c}}{\~a}o de 
                         sub-harm{\^o}nicas e compress{\~a}o de pulsos considerando 
                         pulsos senoidais e de RF. ABSTRACT: In a general formulation 
                         described by a system of ordinary differential equations in the 
                         time domain, this dissertation investigates the propagation 
                         phenomena in linear and nonlinear transmission lines consisting of 
                         LC and LC cells. Important from conceptual point of view but 
                         little discussed in the literature, two mathematical formulations 
                         were developed and then compared. For the first formulation the 
                         state variables were assigned as the mesh current flowing in each 
                         section and the corresponding charge stored in each capacitor. For 
                         the second formulation the inductor current of each section and 
                         the voltage across the capacitors were the state variables 
                         considered. Of importance from the numerical standpoint and since 
                         there are few studies on such formulations, these variables were 
                         adopted so that the differential equations are all first order. 
                         The developed formulation was written so that to each discrete 
                         element in a particular section i values arbitrary L\$_{i}\$ and 
                         C\$_{i}\$ could be assigned. Furthermore, the formulation allows 
                         the analysis of transmission lines being excited by a pulse of 
                         arbitrary shape. In the linear regime, we examined the propagation 
                         characteristics of periodic lines in which the unit cells repeat 
                         themselves periodically, and also doubly periodic lines, where 
                         each odd-numbered section consists of one pair of elements 
                         L\$_{1}\$ and C\$_{1}\$, while the even sections include an 
                         inductor L\$_{2}\$ and a capacitor C\$_{2}\$. In assigning the 
                         values of the circuit elements two cases were considered. For 
                         periodic lines the interpretation of positive and negative phase 
                         velocities, respectively associated to LC and LC topologies, were 
                         highlighted upon considering sinusoidal signals. As for doubly 
                         periodic lines spatial filtering properties were emphasized, since 
                         such lines with lumped elements exhibited strong spatial 
                         dispersion in which each node of the line has a distinct frequency 
                         spectrum. In the nonlinear regime, we investigated some phenomena 
                         associated with the LC line such as RF generation, generation of 
                         solitons, and reduction of the rise and fall times of trapezoidal 
                         pulses propagating along the line. Concerning CL lines we examined 
                         the formation of bright and dark solitons (the latter is a 
                         distinguished feature of CL lines) and also sub-harmonic 
                         generation and pulse compression by considering sinusoidal, 
                         Gaussian, and RF pulses.",
            committee = "Ricci, Mario Cesar (presidente) and Castro, Joaquim Jos{\'e} 
                         Barroso de (orientador) and Rossi, Jos{\'e} Osvaldo (orientador) 
                         and Coutinho, Olympio Lucchini",
         englishtitle = "Modeling and analysis of nonlinear transmission lines with lumped 
                         elements in LC and CL configurations",
             language = "pt",
                pages = "144",
                  ibi = "8JMKD3MGP7W/3FDFFC5",
                  url = "http://urlib.net/ibi/8JMKD3MGP7W/3FDFFC5",
           targetfile = "publicacao.pdf",
        urlaccessdate = "16 jun. 2024"
}


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