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By Kravchenko A.V.

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059 for the square), the light intensity fluctuations are small. For a moderate increase in the cylinder temperature, the vortex strength is enhanced, being accompanied by regular and strong vortex shedding. Therefore, the maximum RMS intensity increases initially with Richardson number. 45 30 30 20 20 10 10 0 0 0 1 2 3 x/d 4 5 6 0 1 2 3 x/d 4 5 6 Fig. 45), Re = 110. 155 30 Irms Irms 30 20 20 10 10 0 0 1 2 3 x/d 4 5 6 0 0 1 2 3 x/d 4 5 6 Fig. 45), Re = 109. Dependence on Richardson number is shown 26 2 Flow Past Heated Bluff Bodies are also weakened.

The first image in the sequence is at the extreme leftward position of the cylinder. Images in Fig. 17a–h show an intense activity in the vicinity of the cylinder as compared to a stationary cylinder, and the vortices from opposite shear layers are inclined toward the wake centreline. 2 Time Traces and Power Spectra The time traces of the light intensity fluctuations in schlieren images is presented here as a function of Richardson number. The cylinder is oscillated at the fundamental frequency (Fig.

This necessitates the use of baffles suspended from the copper sheet that act as fins and maintain the temperature of the lower wall at the desired value. For the top tank, contact area between the flowing water and the copper surface is readily available. 1 K, the tolerance of temperature control obtainable with the constant temperature baths. 4 times the cavity surface area to reduce edge effects. To resolve the near wall intensity variation, the two copper plates have been carefully checked for flatness and surface finish.

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Q -Universal Quasivarieties of Graphs by Kravchenko A.V.


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