strong damping
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2022 ◽  
Vol 2 ◽  
pp. 5
Author(s):  
Ducival C. Pereira ◽  
Geraldo M. de Araújo ◽  
Carlos A. Raposo

In this manuscript, we investigate the unilateral problem for a viscoelastic beam equation of p-Laplacian type. The competition of the strong damping versus the logarithmic source term is considered. We use the potential well theory. Taking into account the initial data is in the stability set created by the Nehari surface, we prove the existence and uniqueness of global solutions by using the penalization method and Faedo-Galerkin’s approximation.


2021 ◽  
Vol 2021 ◽  
pp. 1-11
Author(s):  
Honglv Ma ◽  
Jing Wang ◽  
Jun Xie

In this paper, we obtain the existence of pullback attractors for nonautonomous Kirchhoff equations with strong damping, which covers the case of possible generation of the stiffness coefficient. For this purpose, a necessary method via “the measure of noncompactness” is established.


2021 ◽  
Vol 648 ◽  
pp. A77
Author(s):  
J. M. Riedl ◽  
C. A. Gilchrist-Millar ◽  
T. Van Doorsselaere ◽  
D. B. Jess ◽  
S. D. T. Grant

Context. Solar magnetic pores are, due to their concentrated magnetic fields, suitable guides for magnetoacoustic waves. Recent observations have shown that propagating energy flux in pores is subject to strong damping with height; however, the reason is still unclear. Aims. We investigate possible damping mechanisms numerically to explain the observations. Methods. We performed 2D numerical magnetohydrodynamic (MHD) simulations, starting from an equilibrium model of a single pore inspired by the observed properties. Energy was inserted into the bottom of the domain via different vertical drivers with a period of 30 s. Simulations were performed with both ideal MHD and non-ideal effects. Results. While the analysis of the energy flux for ideal and non-ideal MHD simulations with a plane driver cannot reproduce the observed damping, the numerically predicted damping for a localized driver closely corresponds with the observations. The strong damping in simulations with localized driver was caused by two geometric effects, geometric spreading due to diverging field lines and lateral wave leakage.


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