Abstract

Dicing soft solids with a sharp knife is quicker and smoother if the blade is sliding rapidly parallel to its edge in addition to the normal squeezing motion. We explain this common observation with a consistent theory suited for soft gels and departing from the standard theories of elastic fracture mechanics developed for a century. The gel is assumed to locally fail when submitted to stresses exceeding a threshold σ1σ_1. The changes in its structure generate a liquid layer coating the blade and transmitting the stress through viscous forces. The driving parameters are the ratio U/WU/W of the normal to the tangential velocity of the blade, and the characteristic length ηW/σ1ηW/σ_1, with ηη the viscosity of the liquid. The existence of a maximal value of U/WU/W for a steady regime explains the crucial role of the tangential velocity for slicing biological and other soft materials.

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