Despite being commonly credited (rightly so) with initiating the field of cavitation in elastomers, the famed rubber poker-chip experiments of Gent and Lindley (1959) have yet to be fully explained. One likely reason for their elusiveness is that it had long been presumed that cavitation in elastomers was a phenomenon that could be explained solely on the basis of the elasticity of the elastomer at hand. In the last lustrum, full-field analyses and experiments carried out at high spatiotemporal resolution have debunked such a belief and made plain, instead, that cavitation in elastomers is first and foremost a fracture phenomenon. In that spirit, Kumar, Francfort, and Lopez-Pamies (2018) have introduced a comprehensive macroscopic phase-field theory for the nucleation and propagation of fracture in elastomers undergoing arbitrarily large quasistatic deformations. In this presentation, I will deploy this theory in order to explain in a detailed and quantitative manner the seminal poker-chip experiments of Gent and Lindley.

The poker-chip experiments of Gent and Lindley (1959) explained

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