In this study, a phase-field-based regularized lattice Boltzmann method is proposed to solve axisymmetric two-phase electrohydrodynamic (EHD) flow problems. Three regularized lattice Boltzmann equations are formulated to solve the axisymmetric electric scalar potential equation, the axisymmetric conservation form of the Allen–Cahn phase field equation, and the axisymmetric velocity-based Navier–Stokes equation, respectively. Both the perfect dielectric model and the leaky dielectric model are considered. The accuracy and stability of the proposed regularized lattice Boltzmann model are evaluated through several numerical examples in axisymmetric geometries, including static droplet tests, EHD droplet deformation, EHD Rayleigh–Taylor instability, EHD Rayleigh–Plateau instability, and ionic liquid ferrofluid droplet spreading. The numerical results are in good agreement with existing analytical, experimental, and numerical data. The findings indicate that the presence of the electric field significantly influences the two-phase flow dynamics. For the leaky dielectric model when the conductivity ratio is less than the permittivity ratio, the EHD flow deforms perpendicular to the direction of the electric field. In contrast, in other cases, the EHD flow deforms along the direction of the electric field. In most scenarios, the electric field intensifies the evolution of the two-phase interface and induces complex interfacial hydrodynamic behaviors.
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