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March 5, 2026Journal of Mathematical Physics0 citations

Optimal boundary control of viscoelastic fluids equations

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XYXin YinZTZhong TanJZJianfeng Zhou

Key Points

  • The study aims to explore boundary control in equations governing viscoelastic fluids and establish the conditions for optimal control.
  • Examined equations for viscoelastic rate type fluids and established no-slip boundary conditions.
  • Proved existence of weak solutions for fluid equations and derived uniqueness for weak and strong solutions in 2D.
  • Analyzed the control to state operator's properties in Banach spaces, establishing differentiability.
  • Utilized the Lagrange principle to demonstrate optimality conditions for boundary control.
  • Established weak solutions for the viscoelastic fluid equations under specified conditions.
  • Demonstrated uniqueness of weak and strong solutions in two dimensions.
  • Shown that the control to state operator is Fréchet differentiable.
  • Proved the existence of optimal boundary control and necessary conditions for optimality.

Abstract

In this paper, we consider the equations for viscoelastic rate type fluids, which is viewed as the Navier–Stokes equation coupled with a rate type viscoelastic fluid model. The fluid velocity is assumed to satisfy a no-slip boundary condition, while the extra stress tensor is subject to a time-dependent Dirichlet boundary condition. First we prove the existence of weak solutions to (1.2)–(1.4). If d = 2, we further derive the existence and uniqueness of weak and strong solution. Next, based on the existence of global strong solution, we show that the control to state operator is Fréchet differentiable between appropriate Banach spaces. Finally, by using the properties of the control to state operator and the Lagrange principle, we prove the existence and necessary optimality condition of an optimal boundary control problem.

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Cite This Study

Yin et al. (2026) studied this question.

synapsesocial.com/papers/69a91e1fd6127c7a504c1b8fhttps://doi.org/10.1063/5.0311050
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