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The Penrose-Fife phase-field model with coupled dynamic boundary conditions

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  • In this paper we derive, starting from the basic principles of ther- modynamics, an extended version of the nonconserved Penrose-Fife phase tran- sition model, in which dynamic boundary conditions are considered in order to take into account interactions with walls. Moreover, we study the well- posedness and the asymptotic behavior of the initial-boundary value problem for the PDE system associated to the model, allowing the phase con guration of the material to be described by a singular function.
    Mathematics Subject Classification: 35K61, 35D30, 34B16, 74H40, 34K21, 80A22.

    Citation:

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  • [1]

    H. Attouch, Variational Convergence for Functions and Operators, Applicable Mathematics Series, Pitman (Advanced Publishing Program), Boston, MA, 1984.

    [2]

    V. Barbu, Nonlinear Semigroups and Differential Equations in Banach Spaces, Noordhoff, Leyden, 1976.

    [3]

    M. Bonforte and J.L. Vázquez, Positivity, local smoothing, and Harnack inequalities for very fast diffusion equations, Adv. Math., 223 (2010), 529-578.doi: 10.1016/j.aim.2009.08.021.

    [4]

    H. Brézis, Opérateurs Maximaux Monotones et Semi-groupes de Contractions dans les Éspaces de Hilbert, North-Holland Math. Studies, 5, North-Holland, Amsterdam, 1973.

    [5]

    F. Brezzi and G. Gilardi, FEM Mathematics, in Finite Element Handbook (Ed. H. Kardestuncer), Part I: Chapt. 1: Functional Analysis, 1.1-1.5; Chapt. 2: Functional Spaces, 2.1-2.11; Chapt. 3: Partial Differential Equations, 3.1-3.6, McGraw-Hill Book Co., New York, 1987.

    [6]

    G. Caginalp, An analysis of a phase field model of a free boundary, Arch. Rational Mech. Anal., 92 (1986), 205-245.doi: 10.1007/BF00254827.

    [7]

    C. Cavaterra, C. G. Gal, M. Grasselli and A. Miranville, Phase-field systems with nonlinear coupling and dynamic boundary conditions, Nonlinear Anal., 72 (2010), 2375-2399.doi: 10.1016/j.na.2009.11.002.

    [8]

    L. Cherfils, S. Gatti and A. Miranville, Existence of global solutions to the Caginalp phase-field system with dynamic boundary conditions and singular potentials, J. Math. Anal. Appl., 343 (2008), 557-566; Corrigendum, J. Math. Anal. Appl., 348 (2008), 1029-1030.doi: 10.1016/j.jmaa.2008.01.077.

    [9]

    L. Cherfils and A. Miranville, On the Caginalp system with dynamic boundary conditions and singular potentials, Appl. Math., 54 (2009), 89-115.doi: 10.1007/s10492-009-0008-6.

    [10]

    P. Colli and Ph. Laurençot, Weak solutions to the Penrose-Fife phase field model for a class of admissible heat flux laws, Phys. D, 111 (1998), 311-334.doi: 10.1016/S0167-2789(97)80018-8.

    [11]

    M. Conti, S. Gatti and A. Miranville, Asymptotic behavior of the Caginalp phase-field system with coupled dynamic boundary conditions, Discrete Contin. Dyn. Syst. S, 5 (2012), 485-505.doi: 10.3934/dcdss.2012.5.485.

    [12]

    E. Feireisl and G. Schimperna, Large time behaviour of solutions to Penrose-Fife phase change models, Math. Methods Appl. Sci., 28 (2005), 2117-2132.doi: 10.1002/mma.659.

    [13]

    H. P. Fischer, P. Maass and W. Dieterich, Novel surface modes in spinodal decomposition, Phys. Rev. Letters, 79 (1997), 893-896.doi: 10.1103/PhysRevLett.79.893.

    [14]

    H. P. Fischer, P. Maass and W. Dieterich, Diverging time and length scales of spinodal decomposition modes in thin flows, Europhys. Letters, 42 (1998), 49-54.

    [15]

    H. P. Fischer, J. Reinhard, W. Dieterich, J.-F. Gouyet, P. Maass, A. Majhofer and D. Reinel, Time-dependent density functional theory and the kinetics of lattice gas systems in contact with a wall, J. Chem. Phys., 108 (1998), 3028-3037.doi: 10.1063/1.475690.

    [16]

    C. G. Gal and M. Grasselli, On the asymptotic behavior of the Caginalp system with dynamic boundary conditions, Commun. Pure Appl. Anal., 8 (2009), 689-710.doi: 10.3934/cpaa.2009.8.689.

    [17]

    G. Gilardi, A. Miranville and G. Schimperna, On the Cahn-Hilliard equation with irregular potentials and dynamic boundary conditions, Commun. Pure Appl. Anal., 8 (2009), 881-912.doi: 10.3934/cpaa.2009.8.881.

    [18]

    G. Gilardi, A. Miranville and G. Schimperna, Long time behavior of the Cahn-Hilliard equation with irregular potentials and dynamic boundary conditions, Chin. Ann. Math. Ser. B, 31 (2010), 679-712.doi: 10.1007/s11401-010-0602-7.

    [19]

    G. R. Goldstein, A. Miranville and G. Schimperna, A Cahn-Hilliard model in a domain with non-permeable walls, Phys. D, 240 (2011), 754-766.doi: 10.1016/j.physd.2010.12.007.

    [20]

    M. Grasselli, A. Miranville and G. Schimperna, The Caginalp phase-field system with coupled dynamic boundary conditions and singular potentials, Discrete Contin. Dyn. Syst., 28 (2010), 67-98.doi: 10.3934/dcds.2010.28.67.

    [21]

    M. Grasselli, H. Petzeltová and G. Schimperna, Long time behavior of solutions to the Caginalp system with singular potential, Z. Anal. Anwend., 25 (2006), 51-72.doi: 10.4171/ZAA/1277.

    [22]

    J. K. Hale, Asymptotic Behavior of Dissipative Systems, Mathematical Surveys and Monographs, 25, American Mathematical Society, Providence, RI, 1988.

    [23]

    W. Horn, J. Sprekels and S. Zheng, Global existence of smooth solutions to the Penrose-Fife model for Ising ferromagnets, Adv. Math. Sci. Appl., 6 (1996), 227-241.

    [24]

    A. Ito, N. Kenmochi and M. Kubo, Non-isothermal phase transition models with Neumann boundary conditions, Nonlinear Anal., 53 (2003), 977-996.doi: 10.1016/S0362-546X(03)00032-4.

    [25]

    A. Ito and N. Kenmochi, Inertial set for a phase transition model of Penrose-Fife type, Adv. Math. Sci. Appl., 10 (2000), 353-374.

    [26]

    A. Ito, N. Kenmochi and M. Niezgódka, Phase separation model of Penrose-Fife type with Signorini boundary condition, Adv. Math. Sci. Appl., 17 (2007), 337-356.

    [27]

    R. Kenzler, F. Eurich, P. Maass, B. Rinn, J. Schropp, E. Bohl and W. Dieterich, Phase separation in confined geometries: Solving the Cahn-Hilliard equation with generic boundary conditions, Comput. Phys. Commun., 133 (2001), 139-157.doi: 10.1016/S0010-4655(00)00159-4.

    [28]

    Ph. Laurençot, Solutions to a Penrose-Fife model of phase-field type, J. Math. Anal. Appl., 185 (1994), 262-274.doi: 10.1006/jmaa.1994.1247.

    [29]

    Ph. Laurençot, Weak solutions to a Penrose-Fife model for phase transitions, Adv. Math. Sci. Appl., 5 (1995), 117-138.

    [30]

    J.-L. Lions, Quelques Méthodes de Résolution des Problèmes aux Limites non Linéaires, (French) Dunod, Gauthier-Villars, Paris, 1969.

    [31]

    A. Miranville, Some Mathematical Models in Phase Transition, Lecture Notes, Ravello, 2009.doi: 10.3934/dcdss.2014.7.271.

    [32]

    A. Miranville and S. Zelik, Robust exponential attractors for Cahn-Hilliard type equations with singular potentials, Math. Methods Appl. Sci., 27 (2004), 545-582.doi: 10.1002/mma.464.

    [33]

    A. Miranville and S. Zelik, The Cahn-Hilliard equation with singular potentials and dynamic boundary conditions, Discrete Contin. Dyn. Syst., 28 (2010), 275-310.doi: 10.3934/dcds.2010.28.275.

    [34]

    D. Mugnolo and S. Romanelli, Dirichlet forms for general Wentzell boundary conditions, analytic semigroups, and cosine operator functions, Electron. J. Diff. Equ., 2006, 20 pp. (electronic).

    [35]

    O. Penrose and P. C. Fife, Thermodynamically consistent models of phase-field type for the kinetics of phase transitions, Phys. D, 43 (1990), 44-62.doi: 10.1016/0167-2789(90)90015-H.

    [36]

    E. Rocca and G. Schimperna, Universal attractor for some singular phase transition systems, Phys. D, 192 (2004), 279-307.doi: 10.1016/j.physd.2004.01.024.

    [37]

    E. Rocca and G. Schimperna, Universal attractor for a Penrose-Fife system with special heat flux law, Mediterr. J. Math., 1 (2004), 109-121.doi: 10.1007/s00009-004-0007-5.

    [38]

    G. Savaré and A. Visintin, Variational convergence of nonlinear diffusion equations: Applications to concentrated capacity problems with change of phase, Atti Accad. Naz. Lincei Cl. Sci. Fis. Mat. Natur. Rend. Lincei (9) Mat. Appl., 8 (1997), 49-89.

    [39]

    G. Schimperna, Weak solution to a phase-field transmission problem in a concentrated capacity, Math. Methods Appl. Sci., 22 (1999), 1235-1254.doi: 10.1002/(SICI)1099-1476(19990925)22:14<1235::AID-MMA82>3.0.CO;2-W.

    [40]

    G. Schimperna, Global and exponential attractors for the Penrose-Fife system, Math. Models Methods Appl. Sci., 19 (2009), 969-991.doi: 10.1142/S0218202509003681.

    [41]

    G. Schimperna, A. Segatti and S. Zelik, Asymptotic uniform boundedness of energy solutions to the Penrose-Fife model, J. Evol. Equ., 12 (2012), 863-890.doi: 10.1007/s00028-012-0159-x.

    [42]

    G. Schimperna, A. Segatti, and S. Zelik, On a singular heat equation with dynamic boundary conditions, submitted, arXiv:1302.5026, (2013).

    [43]

    J. Simon, Compact sets in the space $L^p(0,T;B)$, Ann. Mat. Pura Appl. (4), 146 (1987), 65-96.doi: 10.1007/BF01762360.

    [44]

    J. Sprekels and S. Zheng, Global smooth solutions to a thermodynamically consistent model of phase-field type in higher space dimensions, J. Math. Anal. Appl., 176 (1993), 200-223.doi: 10.1006/jmaa.1993.1209.

    [45]

    J. L. Vázquez, Smoothing and Decay Estimates for Nonlinear Diffusion Equations, Oxford Lecture Series in Mathematics and its Applications, 33, Oxford University Press, Oxford, 2006.doi: 10.1093/acprof:oso/9780199202973.001.0001.

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