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Air flow separation at high speed
Authors:BV Korvin-Kroukovsky
Abstract:The resistance coefficient of a body moving in a fluid depends on Reynolds Number R, Mach Number M and the parameter gLU2, which is customarily neglected in view of small weight of the air. Here L denotes a characteristic length; U denotes the body's speed of translation. The author points that dimensional deduction of this parameter does not limit it to the acceleration of gravity, and that the resistance coefficient is affected by the general acceleration to which the air is subjected. Evaluation of the acceleration of the air flowing about spheres puts this parameter in the form LR, where the characteristic length L is interpreted as the mean free molecular path. Large and small spheres were found to have widely different values of the pressure coefficient Δpq for the same Reynolds Number or Mach Number. Here Δp denotes the difference in pressure between front stagnation point and the rear portion of the sphere, and q denotes the dynamic pressure. The plot of Δpq against the parameter LR removes this confusion. The low values of Δpq are found to be associated with LR below a certain critical value, and high values of Δpq with LR above the critical value, which apparently indicates the condition under which the flow separation takes place. Attention is called to the effect of air pressure on the separation as shown by the parameter LR, and its possible bearing on the drag in high altitude flying.
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