Time-dependent lift and drag on a rigid body in a viscous steady linear flow

In a L p -L q setting, the authors in [12] proved the existence and uniqueness of local-in-time strong solutions for the system composed by rigid bodies immersed into a

In the case of the coupled system (2.1.5) with Navier-slip boundary condition the existence result of Leray-Hopf type weak solutions was proved in [GVH14] and existence of

A sensitivity analysis is performed on the additional parameters, showing that only the viscous surface Σ has an influence on transmitted waves in the high frequency regime,

We deal with the case where the fluid equations are the non stationary Stokes system and using the enclosure method, we can recover the convex hull of the obstacle and the distance

We first present the influence of the Reynolds number and particle size on particle distribution for neutrally buoyant particles, and then for the case of particles slightly different

Delort in [1] who proved global- in-time existence of weak solutions for the incompressible Euler equations when the initial vorticity is a compactly supported, bounded Radon

Our result can be contrasted with the result from [13] (see also [14] for a gentle exposition) regarding the controllability of the fluid velocity alone in the case of

In this paper we deal with the issue of the inviscid limit for the system “viscous incompressible fluid + rigid body”, which involves an immersed rigid body moving into a