VISCOELASTICITY AND FLEXIBLE STRUCTURES: EXPLORING THEIR INTERPLAY IN DYNAMIC SYSTEMS

This article delves into the study of elastic structures with viscoelastic boundary conditions, focusing on an elastic thin plate in a bounded domain Ω ⊂ ℝ² with 𝐶²-smooth boundary Γ. The plate is clamped, and memory effects are considered on a subset Γ₀ with positive boundary measure. The vertical deflection 𝑦(𝑥, 𝑡) of this thin elastic plate is governed by a partial differential equation involving wave equations and memory effects. The specific problem can be described by the following equations: 𝑦𝑡𝑡(𝑥, 𝑡) + Δ²𝑦(𝑥, 𝑡) = 0, in Ω × ℝ⁺, (1.1a) 𝑦(𝑥, 𝑡) = ∂𝑣𝑦(𝑥, 𝑡) = 0, on Γ₀ × ℝ⁺, (1.1b) ℬ₁𝑦(𝑥, 𝑡) − ∫₀⁺∞ 𝑔′(𝑠) ∂𝑣[𝑦(𝑥, 𝑡) − 𝑦(𝑥, 𝑡 − 𝑠)]d𝑠 = 0, on Γ₀ × ℝ⁺, (1.1c) ℬ₂𝑦(𝑥, 𝑡) + ∫₀⁺∞ 𝑔′(𝑠)[𝑦(𝑥, 𝑡) − 𝑦(𝑥, 𝑡 − 𝑠)]d𝑠 = 𝑢(𝑥, 𝑡), on Γ₁ × ℝ⁺, (1.1d) 𝑦(𝑥, 0⁺) = 𝑦₀(𝑥), 𝑦𝑡(𝑥, 0⁺) = 𝑦₁(𝑥), (1.1e) 𝑦(𝑥, −𝑠) = 𝜗(𝑥, 𝑡), for 0 < 𝑠 < ∞. (1.1f) This study explores the interplay between elastic structures and viscoelastic boundary conditions, examining the behavior of the thin plate under these specified conditions.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2024-12-03
DOI
https://doi.org/10.5281/zenodo.14266050
Primary Topic
Thermoelastic and Magnetoelastic Phenomena
Type
article
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article

VISCOELASTICITY AND FLEXIBLE STRUCTURES: EXPLORING THEIR INTERPLAY IN DYNAMIC SYSTEMS

Zenodo (CERN European Organization for Nuclear Research)
Thermoelastic and Magnetoelastic Phenomena
article

VISCOELASTICITY AND FLEXIBLE STRUCTURES: EXPLORING THEIR INTERPLAY IN DYNAMIC SYSTEMS

article en

Abstract

This article delves into the study of elastic structures with viscoelastic boundary conditions, focusing on an elastic thin plate in a bounded domain Ω ⊂ ℝ² with 𝐶²-smooth boundary Γ. The plate is clamped, and memory effects are considered on a subset Γ₀ with positive boundary measure. The vertical deflection 𝑦(𝑥, 𝑡) of this thin elastic plate is governed by a partial differential equation involving wave equations and memory effects. The specific problem can be described by the following equations: 𝑦𝑡𝑡(𝑥, 𝑡) + Δ²𝑦(𝑥, 𝑡) = 0, in Ω × ℝ⁺, (1.1a) 𝑦(𝑥, 𝑡) = ∂𝑣𝑦(𝑥, 𝑡) = 0, on Γ₀ × ℝ⁺, (1.1b) ℬ₁𝑦(𝑥, 𝑡) − ∫₀⁺∞ 𝑔′(𝑠) ∂𝑣[𝑦(𝑥, 𝑡) − 𝑦(𝑥, 𝑡 − 𝑠)]d𝑠 = 0, on Γ₀ × ℝ⁺, (1.1c) ℬ₂𝑦(𝑥, 𝑡) + ∫₀⁺∞ 𝑔′(𝑠)[𝑦(𝑥, 𝑡) − 𝑦(𝑥, 𝑡 − 𝑠)]d𝑠 = 𝑢(𝑥, 𝑡), on Γ₁ × ℝ⁺, (1.1d) 𝑦(𝑥, 0⁺) = 𝑦₀(𝑥), 𝑦𝑡(𝑥, 0⁺) = 𝑦₁(𝑥), (1.1e) 𝑦(𝑥, −𝑠) = 𝜗(𝑥, 𝑡), for 0 < 𝑠 < ∞. (1.1f) This study explores the interplay between elastic structures and viscoelastic boundary conditions, examining the behavior of the thin plate under these specified conditions.

Zenodo (CERN European Organization for Nuclear Research)
Towson University (US)
Openalex Percentile: Top 66%
Thermoelastic and Magnetoelastic Phenomena
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