Abstract

We study global orientation dynamics of the Doi–Smoluchowski equation with the Maier–Saupe potential on the sphere, which arises in the modeling of rigid rod-like molecules of polymers. Using the orientation tensor we first reconfirm the structure and number of equilibrium solutions established in [H.L. Liu, H. Zhang, P.W. Zhang, Axial symmetry and classification of stationary solutions of Doi–Onsager equation on the sphere with Maier–Saupe potential, Comm. Math. Sci. 3 (2) (2005) 201–218]. We then examine global orientation dynamics in terms of eigenvalues of the orientation tensor via the Doi closure approximation. It is shown that for small intensity 0 < α < 4 , all states will evolve into the isotropic phase; for large intensity α > 4.5 , all states will evolve into the nematic prolate phase; and for the intermediate intensity 4 < α < 4.5 , an initial state will evolve into either the isotropic phase or the stable phase of two nematic prolate phases, depending on whether such an initial configuration crosses a critical threshold. Moreover, the uniaxial symmetry structure is shown to be preserved in time.

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