“…It was proposed that a modified version of the Johnson-Segalman model [102], incorporating terms accounting for the coupling between the mean micellar length and the shear rate, the dynamics of the mechanical interfaces and the flow-concentration coupling, could be used to model this phenomenon. Subsequent experiments have also demostrated that chaotic flows can be supported by semi-dilute solutions of giant wormlike micelles [88,101,103], dilute, shear-thickening solutions of cylindrical micelles [104], lamellar phases of surfactant solutions [105,106], concentrated colloidal suspensions [107], granular matter [108,109] and foam [110].…”