Wall slip across the jamming transition of soft thermoresponsive particles
Thibaut Divoux, V\'eronique Lapeyre, Val\'erie Ravaine and, S\'ebastien Manneville

TL;DR
This study reveals that wall slip velocity in suspensions of soft particles scales as a power law of the viscous stress relative to the yield stress, with the exponent increasing from 1 to 2 across the jamming transition, unifying previous inconsistent observations.
Contribution
It demonstrates a continuous variation of the slip velocity scaling exponent across the jamming transition in soft particle suspensions, providing a unified framework for understanding wall slip behavior.
Findings
Slip velocity scales as a power law of viscous stress minus yield stress.
Exponent p varies from 1 in dilute to 2 in jammed suspensions.
Scaling law holds across the jamming transition for different packing fractions.
Abstract
Flows of suspensions are often affected by wall slip, that is the fluid velocity in the vicinity of a boundary differs from the wall velocity due to the presence of a lubrication layer. While the slip velocity robustly scales linearly with the stress at the wall in dilute suspensions, there is no consensus regarding denser suspensions that are sheared in the bulk, for which slip velocities have been reported to scale as a with exponents inconsistently ranging between 0 and 2. Here we focus on a suspension of soft thermoresponsive particles and show that actually scales as a power law of the viscous stress , where denotes the yield stress of the bulk material. By tuning the temperature across the jamming transition, we further demonstrate that this scaling holds true over a…
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