The immersed boundary method is one of the most useful computational methods in studying fluid structure interaction. On the other hand, the Immersed Boundary method is also known to require small time steps to maintain stability when solved with an explicit method. Many implicit or approximately im
A comparison of implicit solvers for the immersed boundary equations
β Scribed by Elijah P. Newren; Aaron L. Fogelson; Robert D. Guy; Robert M. Kirby
- Publisher
- Elsevier Science
- Year
- 2008
- Tongue
- English
- Weight
- 271 KB
- Volume
- 197
- Category
- Article
- ISSN
- 0045-7825
No coin nor oath required. For personal study only.
β¦ Synopsis
Explicit time discretizations of the immersed boundary method are known to require small timesteps to maintain stability. A number of implicit methods have been introduced to alleviate this restriction to allow for a more efficient method, but many of these methods still have a stability restriction on the timestep. Furthermore, almost no comparisons have appeared in the literature of the relative computational costs of the implicit methods and the explicit method. A recent paper [E.P. Newren, A.L. Fogelson, R.D. Guy, R.M. Kirby, Unconditionally stable discretizations of the immersed boundary equations, J. Comput. Phys. 222 (2007) 702-719.] addressed the confusion over stability of immersed boundary discretizations. This paper identified the cause of instability in previous immersed boundary discretizations as lack of conservation of energy and introduced a new semi-implicit discretization proven to be unconditionally stable, i.e., it has bounded discrete energy. The current paper addresses the issue of the efficiency of the implicit solvers. Existing and new methods to solve implicit immersed boundary equations are described. Systematic comparisons of computational cost are presented for a number of these solution methods for our stable semi-implicit immersed boundary discretization and an explicit discretization for two distinct test problems. These comparisons show that two of the implicit methods are at least competitive with the explicit method on one test problem and outperform it on the other test problem in which the elastic stiffness of the boundary does not dictate the timescale of the fluid motion.
π SIMILAR VOLUMES
A new stiff ordinary differential equation solver has been devised that separates the unknown variables into a fast group and a slow group. The fast variables are solved using the implicit backwarddifferentiation formulas but with a Jacobian of much smaller dimension than that of the original sitiff
We consider two numerical transparent boundary conditions that have been previously introduced in the literature. The first condition (BPP) was proposed by