Abstract

In this work three branches of Immersed Boundary Methods (IBM) are described and validated for incompressible aerodynamics and fluid-structure interactions. These three approaches are: Cut Cell method, Vortex-Penalization method and Forcing method. Two first techniques are validated for external bluff-body flows and the last one is used for fluid-structure interactions. The paper confirms the ability of this family of numerical schemes for accurate and robust simulation of incompressible flows.

Highlights

  • In this work three branches of Immersed Boundary Methods (IBM) are described and validated for incompressible aerodynamics and fluid-structure interactions

  • The Cut-cell methods, called Cartesian grid methods, focus on the discretization of the equations in the mesh cells cut by the immersed boundary

  • As the boundary conditions are directly imposed, there is no diffusion of the interface fluid-solid. These methods are highly efficient from a computational point of view as it is based on the MAC solver on cartesian grids which has been extensively and successfully used in numerical simulations of turbulent flows, both in the context of direct and Large-Eddy simulations

Read more

Summary

The setting of the problem

We consider a two-dimensional flow past a solid obstacle ΩS ⊂ R2 which is governed by the incompressible Navier-Stokes equations. We denote by ΩF the fluid domain in which the Navier-Stokes equations (2.1)-(2.3) are prescribed so that we have Ω = ΩF ∪ ΩS ∪ ΓS where ΓS = ∂ΩS is the solid boundary. In order to determine the location of each point in the computational domain with respect to the solid boundary ΓS, we use the signed algebraic distance to ΓS, which is given by d : Ω −→ R (x, y) −→ d(x, y). Mesh sizes are defined by : li = xi − xi−1 and hj = yj − yj−1. In order to simplify the notations we denote by dij = d(xi, yj) the algebraic distance of the grid point (xi, yj) to the solid boundary ΓS

Cut-cell method
Time discretization : second-order projection method
The discrete representation of the immersed boundary
A staggered arrangement of the unknowns
Vortex penalization method
Vortex method
Penalization method for the velocity formulation
Penalization method for vorticity formulation
Fluid-Structure interactions with IBM
Lagrangian elasticity of an immersed interface
Immersed boundary model
Flow around a circular cylinder
Cellular motility and parametric instability
Findings
Conclusions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.