This paper establishes the global well-posedness and long-time dynamics of the general Ericksen–Leslie system for isotropic nematic liquid crystals under a constant magnetic field. On the two-dimensional torus , a liquid crystal molecule coincides with itself under rotations by integer multiples of , which results in special boundary conditions. We prove the existence of global-in-time strong solutions by developing novel high-order energy estimates and employing compactness techniques. A key challenge lies in controlling the orientation of the liquid crystal molecules. After achieving a uniform bound for the molecular orientation angle in , we further characterize the long-time behavior of the solutions. This is accomplished by applying the Lojasiewicz–Simon inequality, which reveals the convergence of the solutions as time approaches infinity.

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