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Bryan Quaife
Spectral Deferred Correction Methods for Vesicle Suspensions

University of Texas
Austin
quaife@ices.utexas.edu
George Biros

Vesicles are inextensible capsules filled with and submerged in a viscous fluid. Their dynamics are governed by an internal energy due to bending and tension, a background velocity, and the inextensibility condition. In many simulations, the dynamics can complicate or simplify, and, therefore, we are introducing time adaptivity. In order to allow for large time steps, we are only interested in second- or higher-order methods. Unfortunately, backward difference formulas that use two or more previous time steps can become unstable if the time step size changes too rapidly. Therefore, we iteratively use a first-order method in a spectral deferred correction (SDC) framework to develop high-order solutions that only require the previous time step. The result is a high-order method that remains stable even if the time step size changes rapidly.

The velocity of a vesicle $ j$ , parameterized by $ {\mathbf{x}}_{j}$ with tension $ \sigma_{j}$ , is governed by the integro-differential equation

$\displaystyle &\frac{d{\mathbf{x}}_{j}}{dt} = \sum_{k}{\mathbf{v}}[{\mathbf{x}}_{k}]{\mathbf{x}}_{j},$    

where $ {\mathbf{v}}[{\mathbf{x}}_{k}]{\mathbf{x}}_{j}$ is the velocity due to vesicle $ k$ acting on vesicle $ j$ . A first-order solution $ {\tilde{{\mathbf{x}}}}$ is formed by solving the semi-implicit discretization

$\displaystyle &\frac{{\mathbf{x}}_{j}^{N+1} - {\mathbf{x}}_{j}^{N}}{\Delta t} = \sum_{k}{\mathbf{v}}[{\mathbf{x}}_{k}^{N}]{\mathbf{x}}_{j}^{N+1}.$    

Our SDC formulation forms the higher accurate solution $ {\tilde{{\mathbf{x}}}}+ {\tilde{\boldsymbol{\delta}}}$ where $ {\tilde{\boldsymbol{\delta}}}$ is an approximate solution of

$\displaystyle {\boldsymbol{\delta}}_{j} = \mathbf{e}_{j} + \int_{0}^{t}\sum_{k}...
...\boldsymbol{\delta}}_{k}] ({\mathbf{x}}_{j} + {\boldsymbol{\delta}}_{j}) d\tau,$    

and $ \mathbf{e}$ is the residual of the previous solution. This update can be performed iteratively, and, asymptotically, each iteration increases the formal order of accuracy by one.




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Copper Mountain 2014-02-24