2019
DOI: 10.1177/1748302619861734
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Procedure for 2D fluid–structure interaction simulation

Abstract: A numerical technique for the solution of the structural dynamics equations of motion is presented. The structural dynamics mass and momentum conservation equations are solved using a control volume technique which is secondorder accurate in space along with a dual time-step scheme that is second order accurate in time. The momentum conservation equation is written in terms of the Piola-Kirchoff stresses and the displacement velocity components. The stress tensor is related to the Lagrangian strain and displac… Show more

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Cited by 2 publications
(13 citation statements)
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References 17 publications
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“…7 The proposed solver demonstrated excellent agreement with theoretical vibratory response of a cantilever beam and good agreement with literature. 7,9 The second test case was a highly flexible square cantilever plate subject to a gravitational load. The first two modal frequencies predicted by the presented structural solver show good agreement with the commercial code ANSYS-Discovery AIM.…”
Section: Discussionsupporting
confidence: 68%
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“…7 The proposed solver demonstrated excellent agreement with theoretical vibratory response of a cantilever beam and good agreement with literature. 7,9 The second test case was a highly flexible square cantilever plate subject to a gravitational load. The first two modal frequencies predicted by the presented structural solver show good agreement with the commercial code ANSYS-Discovery AIM.…”
Section: Discussionsupporting
confidence: 68%
“…The maximum X and Y deformation of point A is 0.0381 m and 0.142 m, respectively. Zorn and Davis 7 reported the maximum displacement of 0.022 m and 0.120 m, while Turek and Hron 9 reported 0.029 m and 0.130 m. The discrepancy between maximum reported the displacements by Zorn and Davis, 7 Turek and Hron, 9 and the current study is caused by the three-dimensional effects of the strain equations.…”
Section: Cantilever Beamcontrasting
confidence: 54%
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