Abstract:The existence and uniqueness of Gevrey regularity solutions for the functionalized Cahn-Hilliard (FCH) and Cahn-Hilliard-Willmore (CHW) equations are established. The energy dissipation law yields a uniform-in-time H 2 bound of the solution, and the polynomial patterns of the nonlinear terms enable one to derive a local-in-time solution with Gevrey regularity. A careful calculation reveals that the existence time interval length depends on the H 3 norm of the initial data. A further detailed estimate for the o… Show more
“…We note that the boundary condition (1.6) does not imply ∂ n ∆ 2 φ = 0 on ∂Ω for the solution to problem (1.1)-(1.7) whenever the trace of the normal derivative of ∆ 2 φ makes sense. Thus, we cannot apply the argument in the periodic setting (see [9,57]) to derive a globalin-time estimate on ∇∆φ by testing the phase-field equation (1.3) with −∆ 3 φ (or equivalently, testing the equation (1.4) by ∂ t ∆φ). Actually, we have…”
Section: Local Well-posednessmentioning
confidence: 99%
“…A lot of work has been done to understand morphological changes of membranes. We refer to [2,3,7,8,18-22, 33, 39] for mathematical modeling and numerical simulations, see also [9,11,13,17,23,37,57] for rigorous analysis.…”
Section: Introductionmentioning
confidence: 99%
“…When the fluid coupling is neglected (i.e., setting u = 0 in (1.3)), for the functionalized Cahn-Hilliard equation subject to periodic boundary conditions, the authors of [14] proved the existence of global weak solutions in the case of a regular potential and a degenerate mobility. For η ∈ R, m = 1, and a regular potential, existence and uniqueness of global solutions in the Gevrey class were established in [9], again in the periodic setting. In the recent work [48], the authors considered the case η ∈ R, m = 1 with a physically relevant logarithmic potential 1).…”
In this paper, we study a hydrodynamic phase-field system modeling the deformation of functionalized membranes in incompressible viscous fluids. The governing PDE system consists of the Navier-Stokes equations coupled with a convective sixth-order Cahn-Hilliard type equation driven by the functionalized Cahn-Hilliard free energy, which describes phase separation in mixtures with an amphiphilic structure. In the three dimensional case, we first prove existence of global weak solutions provided that the initial total energy is finite. Then we establish uniqueness of weak solutions under suitable regularity assumptions only imposed on the velocity field (or its gradient). Finally, we prove the existence and uniqueness of local strong solutions for arbitrary regular initial data and derive some blow-up criteria. The results are obtained in the general setting with variable viscosity and mobility.
“…We note that the boundary condition (1.6) does not imply ∂ n ∆ 2 φ = 0 on ∂Ω for the solution to problem (1.1)-(1.7) whenever the trace of the normal derivative of ∆ 2 φ makes sense. Thus, we cannot apply the argument in the periodic setting (see [9,57]) to derive a globalin-time estimate on ∇∆φ by testing the phase-field equation (1.3) with −∆ 3 φ (or equivalently, testing the equation (1.4) by ∂ t ∆φ). Actually, we have…”
Section: Local Well-posednessmentioning
confidence: 99%
“…A lot of work has been done to understand morphological changes of membranes. We refer to [2,3,7,8,18-22, 33, 39] for mathematical modeling and numerical simulations, see also [9,11,13,17,23,37,57] for rigorous analysis.…”
Section: Introductionmentioning
confidence: 99%
“…When the fluid coupling is neglected (i.e., setting u = 0 in (1.3)), for the functionalized Cahn-Hilliard equation subject to periodic boundary conditions, the authors of [14] proved the existence of global weak solutions in the case of a regular potential and a degenerate mobility. For η ∈ R, m = 1, and a regular potential, existence and uniqueness of global solutions in the Gevrey class were established in [9], again in the periodic setting. In the recent work [48], the authors considered the case η ∈ R, m = 1 with a physically relevant logarithmic potential 1).…”
In this paper, we study a hydrodynamic phase-field system modeling the deformation of functionalized membranes in incompressible viscous fluids. The governing PDE system consists of the Navier-Stokes equations coupled with a convective sixth-order Cahn-Hilliard type equation driven by the functionalized Cahn-Hilliard free energy, which describes phase separation in mixtures with an amphiphilic structure. In the three dimensional case, we first prove existence of global weak solutions provided that the initial total energy is finite. Then we establish uniqueness of weak solutions under suitable regularity assumptions only imposed on the velocity field (or its gradient). Finally, we prove the existence and uniqueness of local strong solutions for arbitrary regular initial data and derive some blow-up criteria. The results are obtained in the general setting with variable viscosity and mobility.
“…For the functionalized Cahn-Hilliard equation (i.e., η < 0) subject to periodic boundary conditions, in [14], the authors proved existence of global weak solutions in the case of regular potential and degenerate mobility. Besides, for η ∈ R, M = 1 and a regular potential, existence and uniqueness of global solutions in the Gevrey class were established in [11], again in the periodic setting. We note that in those contributions [11,14,20,31] mentioned above, the potential F is always assumed to be a regular one.…”
Section: Introductionmentioning
confidence: 99%
“…Besides, for η ∈ R, M = 1 and a regular potential, existence and uniqueness of global solutions in the Gevrey class were established in [11], again in the periodic setting. We note that in those contributions [11,14,20,31] mentioned above, the potential F is always assumed to be a regular one. Indeed, this choice plays a crucial role in the mathematical analysis therein.…”
We consider a class of six-order Cahn-Hilliard equations with logarithmic type potential. This system is closely connected with some important phase-field models relevant in different applications, for instance, the functionalized Cahn-Hilliard equation that describes phase separation in mixtures of amphiphilic molecules in solvent, and the Willmore regularization of Cahn-Hilliard equation for anisotropic crystal and epitaxial growth. The singularity of the configuration potential guarantees that the solution always stays in the physical relevant domain [−1, 1]. Meanwhile, the resulting system is characterized by some highly singular diffusion terms that make the mathematical analysis more involved. We prove existence and uniqueness of global weak solutions and show their parabolic regularization property for any positive time. Besides, we investigate longtime behavior of the system, proving existence of the global attractor for the associated dynamical process in a suitable complete metric space.
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