2008
DOI: 10.1051/m2an:2008021
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Numerical solution of a 1-d elastohydrodynamic problem in magnetic storage devices

Abstract: Abstract. In this work we present new numerical methods to simulate the mechanics of head-tape magnetic storage devices. The elastohydrodynamic problem is formulated in terms of a coupled system which is governed by a nonlinear compressible Reynolds equation for the air pressure over the head, and a rod model for the tape displacement. A fixed point algorithm between the solutions of the elastic and hydrodynamic problems is proposed. For the nonlinear Reynolds equation, a characteristics method and a duality a… Show more

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Cited by 9 publications
(8 citation statements)
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“…16.31 202 [2] 13.51 364 [4] 11.59 526 [6] 10.23 688 [8] 9.63 850 [10] 8.76 Table 1: Relative pressure errors for a variety of coarse space dimensions for coefficient with channels and inclusions.…”
Section: Numerical Resultsmentioning
confidence: 99%
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“…16.31 202 [2] 13.51 364 [4] 11.59 526 [6] 10.23 688 [8] 9.63 850 [10] 8.76 Table 1: Relative pressure errors for a variety of coarse space dimensions for coefficient with channels and inclusions.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Note that this condition allows to prove the convergence of the fixed point iteration in [10] for a variational inequality problem. Also, for an elastohydrodynamic problem in magnetic storage devices the convergence is theoretically proved under the same condition in [4]. We also mention that the number of fixed point iteration where chosen to be a constant number independently of of the time step iteration.…”
Section: A Duality Methods For Nonlinear Termsmentioning
confidence: 92%
“…The tape deflection u is given by a fourth order linear equation of Euler-Bernoulli Beam equation type (see [4], [9,Chap. 6] and [1]). The position of the tape "u" is given by the beam equation, (see [4], [9,Chap.6] for details).…”
Section: Modellingmentioning
confidence: 99%
“…In order to compute the solution we reformulate the problem in terms of an obstacle one relative to the unknown h = u − δ, so that we can guarantee that h > 0, that is to say, the tape keeps above the head. We shall follow the ideas of [1,2], and apply a finite element method together with a duality algorithm handling Yosida approximation tools for maximal monotone operators. These techniques have already been successfully used for example in [7] and [8].…”
Section: Numerical Resolutionmentioning
confidence: 99%
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