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29. On the importance of accurately resolving negative pressures in SPH simulations of complex fluid structure interaction problems

30. Towards the modelling of underwater-explosion or cavitation bubbles: proposal of a compressible multiphase SPH model

31. Simulations of airplane and helicopter ditching using Smoothed Particle Hydrodynamics

32. Study of the time-step ratio between SPH and FE solvers for FSI problems

33. Derivation and validation of δ-SPH model for simulating strongly-compressible multiphase flows

34. A higher order SPH scheme based on WENO reconstructions for two-dimensional problems

35. Experimental design and simulation of helicopter ditching

36. Multiple bifurcations of the flow over stalled airfoils when changing the Reynolds number

37. How to derive the multi-fluid delta-SPH model

38. Numerical simulations of airplane and helicopter ditching applied to the design of experiments

39. Simulation of a fixed cylinder in waves using the SWENSE method within a weakly-compressible approach

40. Effects of particle disordering on local and global fluid volume in the SPH method and proposition of an improved SPH-ALE scheme

41. Use of WENO reconstructions in a high-order Riemann-SPH scheme

42. A VOF-based finite volume method for numerical simulation of weakly-compressible two-phase flows using higher order schemes

43. Importance of a high-order spatial scheme for the simulation of tidal turbine wakes

44. Development and improvement of a Cartesian solver with immersed boundaries for hydrodynamics

45. Development of a high-order Finite Volume method on Cartesian grids with local grid refinement for hydrodynamics

46. Development of the SWENSE method in a weakly-compressible Cartesian grid approach

47. Development of a coupling strategy between Smoothed Particle Hydrodynamics and Finite Element Method for violent fluid-structure interaction problems

48. Particle refinement applied to SPH method : stability, accuracy and CPU analysis

50. Improvements on Particle Refinement method with SPH

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