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A typical example of shock wave boundary layer interaction is the flowfield past aerodynamic surfaces during control.
The aerothermodynamic loadings associated with shock wave boundary layer interactions (shock interactions) must be carefully considered in the design of hypersonic air vehicles.
Shock wave boundary layer interaction (SWBLI) is most attended research theme in the high speed flow regime for effective design of various parts of space vehicles.
The edge of the bottom wave boundary layer is estimated to be located at one Nikuradse roughness length above the level midway between crest and trough of the ripples.
In the present work, the open source Computational Fluid Dynamics (CFD) package-Open Field Operation and Manipulation (OpenFoam®) is used to simulate wave-structure interactions and a new wave boundary condition is developed for extreme waves.
In this paper, an inverse method to calculate the band structure of one dimensional periodic structures based on Bloch wave boundary conditions and wave superposition is introduced.
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Such methods rely heavily on the accuracy of fiducial detection, which is still an open problem due to the difficulty in exact localization of wave boundaries.
The methods incorporating time and amplitude characteristics of the heartbeats strongly rely on the correct localization of wave boundaries within the P-QRS-T segment.
This work uses the hard-sphere model to simulate the particle motion pattern in a two-dimensional rotating tumbler with a sine-wave boundary.
In particular, we investigate the reconstruction and the prediction of shock waves, boundary layers and vortices.
In recent years, the fractional differential equations have been used in various fields such as colored noise, electromagnetic waves, boundary layer effects in ducts, viscoelastic mechanics, diffusion processes, and so on [1 5].
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