2005
DOI: 10.1007/s10573-005-0008-0
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Drag of nonspherical particles in a flow behind a shock wave

Abstract: The early stage of velocity relaxation of nonspherical particles in a flow behind an incident shock wave is considered by the method of multiframe shadowgraphy. A procedure of processing the data on the motion of a free body for determining its acceleration is proposed; in combination with the diagnostic method used, the procedure forms something like a noncontact aerodynamic balance. Novel data on the drag of bodies of irregular shape in a flow behind a shock wave with Mach numbers of 0.5-1.5 and Reynolds num… Show more

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Cited by 16 publications
(36 citation statements)
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“…It was shown [12][13][14] that the definition of the drag coefficient C D = 2F a /sρu 2 and the equation of particle motion in the flow behind the shock wave…”
Section: Dynamics Of the Drop In The Flow Behind The Shock Wave And Tmentioning
confidence: 99%
See 2 more Smart Citations
“…It was shown [12][13][14] that the definition of the drag coefficient C D = 2F a /sρu 2 and the equation of particle motion in the flow behind the shock wave…”
Section: Dynamics Of the Drop In The Flow Behind The Shock Wave And Tmentioning
confidence: 99%
“…It was experimentally demonstrated [14] that dependence (3) provides an accurate description of particle motion in the SW until the time θ ≈ 1 and, hence, can be used for approximation of experimental data in finding C D . The value of λ is found from the condition of the best approximation, and Eq.…”
Section: Dynamics Of the Drop In The Flow Behind The Shock Wave And Tmentioning
confidence: 99%
See 1 more Smart Citation
“…Boiko and Poplavski [7] performed experiments on acceleration of balsa particles in gas flows with Mach numbers 0.5-1.5. To process the experimental results, they assumed that the drag coefficient was constant.…”
Section: Introductionmentioning
confidence: 99%
“…To process the experimental results, they assumed that the drag coefficient was constant. Its value was found on the basis of the exact solution of the equation of motion for a particle located in the gas flow behind the SW. Boiko and Poplavski [7] considered the value of C D obtained as a result of averaging during the observation time.…”
Section: Introductionmentioning
confidence: 99%