Stability and Energy Decay for a Porous-Elastic System with One Global Fractional Damping

In this paper, we study the stability and the energy decay for a porous-elastic system with one global fractional damping. First, by the Lumer–Phillips theorem, we show that the system is well posed. Then, by the general criteria of Arendt–Batty, we show that the system is strongly stable. Finally, by the frequency-domain method, we show that the system is polynomially stable and that the corresponding energy decay rate depends on the wave speeds μρ,δJ and the parameters α,η in the Caputo fractional derivative operator. Specifically, if μρ=δJ and η>0, the optimal energy decay rate of the system is t−21−α; if μρ≠δJ and η>0, the optimal energy decay rate of the system is t−23−α; if μρ=δJ and η=0, the energy decay rate of the system is t−2; if μρ≠δJ and η=0, the energy decay rate of the system is t−23−α.

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Publication Details

Journal
Mathematics
Published
2026-10-27
DOI
https://doi.org/10.3390/math14213919
Primary Topic
Stability and Controllability of Differential Equations
Type
article
Field-Weighted Citation Impact
0.00

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Stability and Energy Decay for a Porous-Elastic System with One Global Fractional Damping

Shuhan Qian, Hualei Zhang, Liao Li
6 links
Mathematics
Stability and Controllability of Differential Equations
article

Stability and Energy Decay for a Porous-Elastic System with One Global Fractional Damping

Shuhan Qian, Hualei Zhang, Liao Li
article en

Abstract

In this paper, we study the stability and the energy decay for a porous-elastic system with one global fractional damping. First, by the Lumer–Phillips theorem, we show that the system is well posed. Then, by the general criteria of Arendt–Batty, we show that the system is strongly stable. Finally, by the frequency-domain method, we show that the system is polynomially stable and that the corresponding energy decay rate depends on the wave speeds μρ,δJ and the parameters α,η in the Caputo fractional derivative operator. Specifically, if μρ=δJ and η>0, the optimal energy decay rate of the system is t−21−α; if μρ≠δJ and η>0, the optimal energy decay rate of the system is t−23−α; if μρ=δJ and η=0, the energy decay rate of the system is t−2; if μρ≠δJ and η=0, the energy decay rate of the system is t−23−α.

MathematicsVol. 14(21)
Shaanxi University of Technology (CN)
Education Department of Shaanxi Province
Openalex Percentile: Top 17%
Stability and Controllability of Differential Equations
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