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Titlebook: Bluff-Body Wakes, Dynamics and Instabilities; IUTAM Symposium, Göt Helmut Eckelmann,J. Michael R. Graham,Peter A. Mon Conference proceeding

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analyses, numerical simulations and turbulence modelling.The main originality of thisvolume is that recentconceptual advances made to describe nonlinearphenomena ingeneral are put to the test on a classical problem infundamental fluid mechanics, namely the wake structuregenerated behind a bluff object.978-3-662-00416-6978-3-662-00414-2
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f recentresultsobtained in the study of bluff-body wakes.Experimental,theoretical and numerical approaches are allcomprehensivelycovered and compared. Topics of particular interest includehydrodynamic instability analyses, three-dimensionalpatternformation problems, flow control methods, bifurcation
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Deterministic Phase Retrieval Using the LCTperiment. The numerical method is based on a viscous vortex (particle) method. The experimental investigation involves the towing of a cylinder through waves in a laboratory flume, and comparison of the transverse force with a quasi-steady model.
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https://doi.org/10.1007/978-1-4615-0553-2 at a reasonable distance from the cylinder, radiative boundary conditions produce results which compare well with the experimental observations, also if the external boundary is quite close to the cylinder.
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https://doi.org/10.1007/978-1-4615-0553-2urrent in the fluid. This current in turn leads (due to its interaction with the magnetic field) to an electromagnetic body force acting on the fluid. In addition the induced current yields a small perturbation of the external magnetic field.
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University Series in Mathematics until the steady state wake oscillation was established. The velocity time traces in the wake taken with a LDV were analyzed using a wavelet analysis technique, and time scales of vortical structures were identified and correlated with the flow visualizations.
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https://doi.org/10.1007/978-1-4615-0553-2sing yaw angle. The pressure behind the cylinder decreases greatly towards the upstream endplate of the cylinder, although there is a strong wedge-shaped recovery of pressure in the region near the rear stagnation. The strong secondary flow behind the yawed circular cylinder is responsible for the recovery region.
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