FLUID On PubPhys: open In the literature: partially resolved Compiled by AI, not yet reviewed by an editor

Threshold speed for air entrainment in forced wetting

In plain words

When a plate or tape is pushed quickly into a liquid, above a critical speed the liquid can no longer wet the solid and a thin air film is dragged in, which ruins coatings. What sets that critical speed?

Precise statement

For a solid plunging at speed $U$ into a liquid of viscosity $\eta$ and surface tension $\gamma$, surrounded by gas of viscosity $\eta_g$ and pressure $p$, predict the critical capillary number $\mathrm{Ca}* = \eta U*/\gamma$ for dynamic wetting failure, including its dependence on the viscosity ratio $\eta_g/\eta$, on gas rarefaction when the mean free path approaches the air-film thickness, and on the large increase of $\mathrm{Ca}*$ when the flow pushes the liquid against the solid (curtain coating). An answer predicts $\mathrm{Ca}*$ within experimental error for $\eta_g/\eta$ from $10^{-6}$ to $10^{-2}$ and across reduced gas pressures.

What would settle it

A comparison of measured $\mathrm{Ca}*$ for plunging plates and curtain coating over wide viscosity ratios and gas pressures with a single model of the gas film and the contact line.

Status in the literature

Unverified note: it names recent work and was partly written without a live literature search; it awaits a check by an editor.

Lubrication models that include gas viscosity capture the weak viscosity-ratio dependence for simple plunging; the roles of gas rarefaction and of flow assistance remain unsettled as of 2026 (not re-verified for 2024-2026).

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