Periodic Oscillations in MEMS under Squeeze Film Damping Force

We provide sufficient conditions for the existence of periodic solutions for an idealized electrostatic actuator modeled by the Liénard-type equation x¨+FDx,ẋ+x=βV2t/1−x2,x∈−∞,1 with β∈ℝ+, V∈Cℝ/Tℤ, and FDx,ẋ=κẋ/1−x3, κ∈ℝ+ (called squeeze film damping force), or FDx,ẋ=cẋ, c∈ℝ+ (called linear dam...

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Main Authors: Juan Beron, Andrés Rivera
Format: Article
Language:English
Published: Wiley 2022-01-01
Series:Journal of Applied Mathematics
Online Access:http://dx.doi.org/10.1155/2022/1498981
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author Juan Beron
Andrés Rivera
author_facet Juan Beron
Andrés Rivera
author_sort Juan Beron
collection DOAJ
description We provide sufficient conditions for the existence of periodic solutions for an idealized electrostatic actuator modeled by the Liénard-type equation x¨+FDx,ẋ+x=βV2t/1−x2,x∈−∞,1 with β∈ℝ+, V∈Cℝ/Tℤ, and FDx,ẋ=κẋ/1−x3, κ∈ℝ+ (called squeeze film damping force), or FDx,ẋ=cẋ, c∈ℝ+ (called linear damping force). If FD is of squeeze film type, we have proven that there exists at least two positive periodic solutions, one of them locally asymptotically stable. Meanwhile, if FD is a linear damping force, we have proven that there are only two positive periodic solutions. One is unstable, and the other is locally exponentially asymptotically stable with rate of decay of c/2. Our technique can be applied to a class of Liénard equations that model several microelectromechanical system devices, including the comb-drive finger model and torsional actuators.
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spelling doaj-art-92aafa75604a4393847d9b18ea4974fc2025-02-03T06:05:02ZengWileyJournal of Applied Mathematics1687-00422022-01-01202210.1155/2022/1498981Periodic Oscillations in MEMS under Squeeze Film Damping ForceJuan Beron0Andrés Rivera1Departamento de Ciencias Naturales y Matemáticas Pontificia Universidad Javeriana CaliDepartamento de Ciencias Naturales y Matemáticas Pontificia Universidad Javeriana CaliWe provide sufficient conditions for the existence of periodic solutions for an idealized electrostatic actuator modeled by the Liénard-type equation x¨+FDx,ẋ+x=βV2t/1−x2,x∈−∞,1 with β∈ℝ+, V∈Cℝ/Tℤ, and FDx,ẋ=κẋ/1−x3, κ∈ℝ+ (called squeeze film damping force), or FDx,ẋ=cẋ, c∈ℝ+ (called linear damping force). If FD is of squeeze film type, we have proven that there exists at least two positive periodic solutions, one of them locally asymptotically stable. Meanwhile, if FD is a linear damping force, we have proven that there are only two positive periodic solutions. One is unstable, and the other is locally exponentially asymptotically stable with rate of decay of c/2. Our technique can be applied to a class of Liénard equations that model several microelectromechanical system devices, including the comb-drive finger model and torsional actuators.http://dx.doi.org/10.1155/2022/1498981
spellingShingle Juan Beron
Andrés Rivera
Periodic Oscillations in MEMS under Squeeze Film Damping Force
Journal of Applied Mathematics
title Periodic Oscillations in MEMS under Squeeze Film Damping Force
title_full Periodic Oscillations in MEMS under Squeeze Film Damping Force
title_fullStr Periodic Oscillations in MEMS under Squeeze Film Damping Force
title_full_unstemmed Periodic Oscillations in MEMS under Squeeze Film Damping Force
title_short Periodic Oscillations in MEMS under Squeeze Film Damping Force
title_sort periodic oscillations in mems under squeeze film damping force
url http://dx.doi.org/10.1155/2022/1498981
work_keys_str_mv AT juanberon periodicoscillationsinmemsundersqueezefilmdampingforce
AT andresrivera periodicoscillationsinmemsundersqueezefilmdampingforce