(S.76) Stream function is (Table S1): 1 4 24 2( ' ) 6 2' sin 36 ' ' gR r r R R R                                 

The internal liquid 1 22( ' ) 6 2' 3 1 cos3 ' 'r gR rV R R                            , (S

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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 43
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.

(S.76) Stream function is (Table S1): 1 4 24 2( ' ) 6 2' sin 36 ' ' gR r r R R R                                 

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