(63) Stream function is   12 24 2( ' ) 6 2, sin 3 6 ' gR r r R rr R R R r R                                           

The external liquid (r > R) 1 32( ' ) 6 2 1 3 1 cos3 'r gR R RV r R r                                   , (61) 1 32( ' ) 6 2 2 3 2 sin6

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Tangential and normal partial slip at the liquid-fluid interfaces: application to a small liquid droplet, gas bubble, and aerosol

physics.flu-dyn · 2026-04-20 · unverdicted · novelty 5.0

Analytical generalization of the Hadamard-Rybczynski equation for droplet and bubble terminal velocity incorporating independent slip lengths for tangential and normal slip at fluid-fluid interfaces.

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Tangential and normal partial slip at the liquid-fluid interfaces: application to a small liquid droplet, gas bubble, and aerosol physics.flu-dyn · 2026-04-20 · unverdicted · none · ref 2
Analytical generalization of the Hadamard-Rybczynski equation for droplet and bubble terminal velocity incorporating independent slip lengths for tangential and normal slip at fluid-fluid interfaces.

(63) Stream function is   12 24 2( ' ) 6 2, sin 3 6 ' gR r r R rr R R R r R                                           

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