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Revision as of 16:27, 27 February 2018 by Himpe (talk | contribs) (Added Circular Piston Benchmark)
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Description: Axi-Symmetric Infinite Element Model for Circular Piston

This example is a model of the form


 M\ddot{x}(t) + E\dot{x}(t) + Kx(t) = f,

with M, C, and K non-symmetric matrices and M singular. This is thus a differential algebraic equation. It is shown that it has index [1]. The input of the system is f, the output is the state vector x. The motivation for using model reduction for this type of problems is the reduction of the computation time of a simulation.

This is an example from an acoustic radiation problem discussed in [2]. Consider a circular piston subtending a polar angle 0<\theta<\theta_p on a submerged massless and rigid sphere of radius \delta. The piston vibrates harmonically with a uniform radial acceleration. The surrounding acoustic domain is unbounded and is characterized by its density \rho and sound speed c.

We denote by p and a_r the prescribed pressure and normal acceleration respectively. In order to have a steady state solution \tilde{p}(r,\theta,t) verifying


\tilde{p}(r,\theta,t) = \mathcal{R} e (p(r,\theta) e^{i\omega t})

the transient boundary condition is chosen as:


a_r = \frac{-1}{\rho} \frac{\partial p(r,\theta)}{\partial r} \big|_{r=a} = \begin{cases} a_0 \sin(\omega t) & 0<\theta<\theta_p \\ 0 & \theta>\theta_p \end{cases}

The axi-symmetric discrete finite-infinite element model relies on a mesh of linear quadrangle finite elements for the inner domain (region between spherical surfaces r=\delta and r=1.5\delta). The numbers of divisions along radial and circumferential directions are 5 and 80, respectively. The outer domain relies on conjugated infinite elements of order 5. For this example we used \delta=1 [m], \rho=1.225 [kg/m^3], c=340 [m/s], a_0 = 0.001 [m/s^2] and \omega = 1000 [rad/s].

The matrices K, C, M and the right-hand side f are computed by Free Field Technologies. The dimension of the second-order system is N=2025.

Origin

This benchmark is part of the Oberwolfach Benchmark Collection[3]; No. 38890.

Data

Download matrices in the Matrix Market format piston.tar.gz (1.9 MB).

References

  1. J.-P. Coyette, K. Meerbergen, M. Robbé, Time integration for spherical acoustic finite-infinite element models, Numerical Methods in Engineering 64(13): 1752--1768, 2003.
  2. P.M. Pinsky and N.N. Abboud, Finite element solution of the transient exterior structural acoustics problem based on the use of radially asymptotic boundary conditions, Computer Methods in Applied Mechanics and Engineering, 85: 311--348, 1991.
  3. J.G. Korvink, E.B. Rudnyi, Oberwolfach Benchmark Collection, Dimension Reduction of Large-Scale Systems, Lecture Notes in Computational Science and Engineering, vol 45: 311--315, 2005.