pith. sign in

For detailed information, see Mukhopadhyay & Mukhopadhyay [36]

If we choose the viscous gravity length scalel ν =ν 2/3(gsinθ) −1/3 andt ν =ν 1/3(gsinθ) −2/3, the velocity scale ˆV=U N = (gsinθ ˆh2 N /ν)(1 + 2β), we getRe/F r 2 = 1/(1 + 2β) [25] · 2000

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it
browse 1 citing papers

fields

physics.flu-dyn 1

years

2026 1

verdicts

UNVERDICTED 1

representative citing papers

Solutocapillary instability in slipping falling films

physics.flu-dyn · 2026-05-17 · unverdicted · novelty 5.0

Wall slip in surfactant-laden falling films produces non-monotonic critical Reynolds numbers with equilibrium coverage, drives a single-to-double-hump transition in solitary waves, and resolves spurious interfacial mass growth via a revised conservative surface balance.

citing papers explorer

Showing 1 of 1 citing paper.

  • Solutocapillary instability in slipping falling films physics.flu-dyn · 2026-05-17 · unverdicted · none · ref 5

    Wall slip in surfactant-laden falling films produces non-monotonic critical Reynolds numbers with equilibrium coverage, drives a single-to-double-hump transition in solitary waves, and resolves spurious interfacial mass growth via a revised conservative surface balance.