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Dispersed phase motion in laminar boundary layer flow over a wedge

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Abstract

The motion of a dispersed phase in the laminar boundary layer on a wedge is considered with allowance for the effect of not only the Stokes force, which coincides in direction with the flow velocity, but also the transverse force (Saffman force) resulting from the transverse nonuniforrnity of the flow over the individual particle [1–3].

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Authors and Affiliations

  1. Moscow

    E. S. Asmolov

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  1. E. S. Asmolov
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Translated from Izvestiya Rossiiskoi Akademii Nauk, Mekhanika Zhidkosti i Gaza, No.6, pp. 34–42, November–December, 1993.

In conclusion, the authors wishes to thank S. V. Manuilovich for assisting with the numerical calculations.

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Asmolov, E.S. Dispersed phase motion in laminar boundary layer flow over a wedge. Fluid Dyn 28, 778–784 (1993). https://doi.org/10.1007/BF01049778

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  • DOI: https://doi.org/10.1007/BF01049778

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