“…In the past couple of decades, there has been a growing interest in investigating droplet dynamics under electrical field, broadly under the scope of droplet electrohydrodynamics (EHD), via extensive theoretical, experimental, and numerical investigations. [32][33][34][35][36][37][38][39][40][41] In electrically mediated flows, droplet breakup is a well-known phenomenon, [42][43][44][45][46][47][48] preceding large deformation at high electrical capillary number, Ca E , signifying a decisive dominance of the electric stress over capillary stress. Fundamentally, in electric field, the droplet deforms to a new shape that is typically characterized by a discriminating function f T (R, S, l), originally introduced by Taylor, 49 where R, S and l are the ratios of electrical conductivity, permittivity and viscosity, respectively, of the droplet and the continuous phase.…”