Using bifurcations in the determination of lock-in ranges for third-order phase-locked loops


Autoria(s): PIQUEIRA, Jose Roberto Castilho
Contribuinte(s)

UNIVERSIDADE DE SÃO PAULO

Data(s)

18/10/2012

18/10/2012

2009

Resumo

Transmission and switching in digital telecommunication networks require distribution of precise time signals among the nodes. Commercial systems usually adopt a master-slave (MS) clock distribution strategy building slave nodes with phase-locked loop (PLL) circuits. PLLs are responsible for synchronizing their local oscillations with signals from master nodes, providing reliable clocks in all nodes. The dynamics of a PLL is described by an ordinary nonlinear differential equation, with order one plus the order of its internal linear low-pass filter. Second-order loops are commonly used because their synchronous state is asymptotically stable and the lock-in range and design parameters are expressed by a linear equivalent system [Gardner FM. Phaselock techniques. New York: John Wiley & Sons: 1979]. In spite of being simple and robust, second-order PLLs frequently present double-frequency terms in PD output and it is very difficult to adapt a first-order filter in order to cut off these components [Piqueira JRC, Monteiro LHA. Considering second-harmonic terms in the operation of the phase detector for second order phase-locked loop. IEEE Trans Circuits Syst [2003;50(6):805-9; Piqueira JRC, Monteiro LHA. All-pole phase-locked loops: calculating lock-in range by using Evan`s root-locus. Int J Control 2006;79(7):822-9]. Consequently, higher-order filters are used, resulting in nonlinear loops with order greater than 2. Such systems, due to high order and nonlinear terms, depending on parameters combinations, can present some undesirable behaviors, resulting from bifurcations, as error oscillation and chaos, decreasing synchronization ranges. In this work, we consider a second-order Sallen-Key loop filter [van Valkenburg ME. Analog filter design. New York: Holt, Rinehart & Winston; 1982] implying a third order PLL The resulting lock-in range of the third-order PLL is determined by two bifurcation conditions: a saddle-node and a Hopf. (C) 2008 Elsevier B.V. All rights reserved.

Identificador

COMMUNICATIONS IN NONLINEAR SCIENCE AND NUMERICAL SIMULATION, v.14, n.5, p.2328-2335, 2009

1007-5704

http://producao.usp.br/handle/BDPI/18706

10.1016/j.cnsns.2008.06.012

http://dx.doi.org/10.1016/j.cnsns.2008.06.012

Idioma(s)

eng

Publicador

ELSEVIER SCIENCE BV

Relação

Communications in Nonlinear Science and Numerical Simulation

Direitos

closedAccess

Copyright ELSEVIER SCIENCE BV

Palavras-Chave #Bifurcation #Lock-in range #Phase-error #Phase-locked loop #Synchronous state #Stability #NETWORK SYNCHRONIZATION #OPERATION #JITTER #Literature, British Isles #Mathematics, Applied #Mathematics, Interdisciplinary Applications #Mechanics #Physics, Fluids & Plasmas #Physics, Mathematical
Tipo

article

original article

publishedVersion