2013
DOI: 10.1016/j.jfluidstructs.2013.05.012
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Oblique water entry of a cone by a fully three-dimensional nonlinear method

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Cited by 44 publications
(15 citation statements)
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“…Due to the horizontal velocity in the x direction, the slope of the pressure curve in the y = 0 plane is no longer zero at the tip, as shown in figure 7(a), while it is still zero in the x = 0 plane, clearly because of the symmetry about the y = 0 plane. In contrast to the discontinuity and sharp variation at the tip of a cone (Sun & Wu 2013a), the pressure here is finite and continuous at the tip. In the vertical entry case, the peak pressure for λ = 1 is at the tip of the body, as shown in figure 5(a).…”
Section: Oblique Water Entrymentioning
confidence: 86%
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“…Due to the horizontal velocity in the x direction, the slope of the pressure curve in the y = 0 plane is no longer zero at the tip, as shown in figure 7(a), while it is still zero in the x = 0 plane, clearly because of the symmetry about the y = 0 plane. In contrast to the discontinuity and sharp variation at the tip of a cone (Sun & Wu 2013a), the pressure here is finite and continuous at the tip. In the vertical entry case, the peak pressure for λ = 1 is at the tip of the body, as shown in figure 5(a).…”
Section: Oblique Water Entrymentioning
confidence: 86%
“…This problem was also solved by Battistin & Iafrati (2003) and by Xu, Duan & Wu (2011). In three dimensions, Sun & Wu (2013a) considered the oblique water entry of a cone and subsequently (in Sun & Wu 2013b) solved the problem of water entry of non-axisymmetric bodies with varying speed. While the above research on self-similar problems has provided significant insight into fluid-structure impact phenomena, the shapes of the solid surface in all these works are limited.…”
Section: Introductionmentioning
confidence: 99%
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“…(19) can also be obtained by using the auxiliary function technique Taylor, 1996, 2003), the details can be found in Wu and Hu (2005) and Sun & Wu (2013, 2014. The hydrodynamic force can be obtained through integrating the pressure along the body surface.…”
Section: Hydrodynamic Pressure and Forcementioning
confidence: 99%
“…There are mainly three numerical schemes to track the free surface of the flooding flow which are boundary element method, smoothed particle hydrodynamics (SPH) method, and volume of fluid (VOF) method [8]. Using the dynamic and kinematic conditions on free surface, the boundary element method usually employed a time stepping scheme to track the free surface based on nonviscosity assumption [20]. The SPH method offers a variety of advantages for fluid modelling, particularly for the splashing droplets problem [21,22].…”
Section: Introductionmentioning
confidence: 99%