Thermal control of a rate-independent model for permanent inelastic effects in shape memory materials

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September 2014, 3(3): 411-427. doi: 10.3934/eect.2014.3.411

Thermal control of a rate-independent model for permanent inelastic effects in shape memory materials

Michela Eleuteri ^1, and Luca Lussardi ^2,

1.	Dipartimento di Matematica e Informatica, Università di Firenze, viale Morgagni 67/a, I-50134 Firenze, Italy
2.	Dipartimento di Matematica e Fisica "N.Tartaglia", Università Cattolica del Sacro Cuore, Via dei Musei 41, I-25121 Brescia, Italy

Received April 2013 Revised January 2014 Published August 2014

Abstract
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We address the thermal control of the quasi-static evolution of a polycrystalline shape memory alloy specimen. The thermomechanical evolution of the body is described by means of an extension of the phenomenological Souza-Auricchio model [6,7,8,57] accounting also for permanent inelastic effects [9,11,27]. By assuming to be able to control the temperature of the body in time we determine the corresponding quasi-static evolution in the energetic sense. In a similar way as in [28], using results by Rindler [49,50] we prove the existence of optimal controls for a suitably large class of cost functionals.

Keywords: permanent inelasticity., rate-independent, Shape memory alloys, optimal control, quasi-static evolution.

Mathematics Subject Classification: 74C05, 49J2.

Citation: Michela Eleuteri, Luca Lussardi. Thermal control of a rate-independent model for permanent inelastic effects in shape memory materials. Evolution Equations and Control Theory, 2014, 3 (3) : 411-427. doi: 10.3934/eect.2014.3.411

References:

[1]	T. Aiki and N. Kenmochi, Some models for shape memory alloys, Mathematical aspects of modelling structure formation phenomena, GAKUTO Internat. Ser. Math. Sci. Appl., Tokio, 17 (2002), 144-162.
[2]	M. Arndt, M. Griebel and T. Roubíček, Modelling and numerical simulation of martensitic transformation in shape memory alloys, Contin. Mech. Thermodyn., 15 (2003), 463-485. doi: 10.1007/s00161-003-0127-3.
[3]	F. Auricchio, A.-L. Bessoud, A. Reali and U. Stefanelli, A phenomenological model for the magneto-mechanical response of single-crystal magnetic shape memory alloys, Preprint IMATI-CNR 3PV13/3/0, 2013.
[4]	F. Auricchio, A.-L. Bessoud, A. Reali and U. Stefanelli, A three-dimensional phenomenological models for magnetic shape memory alloys, GAMM-Mitt., 34 (2011), 90-96. doi: 10.1002/gamm.201110014.
[5]	F. Auricchio, A. Mielke and U. Stefanelli, A rate-independent model for the isothermal quasi-static evolution of shape-memory materials, Math. Models Meth. Appl. Sci., 18 (2008), 125-164. doi: 10.1142/S0218202508002632.
[6]	F. Auricchio and L. Petrini, Improvements and algorithmical considerations on a recent three-dimensional model describing stress-induced solid phase transformations, Internat. J. Numer. Methods Engrg., 55 (2002), 1255-1284. doi: 10.1002/nme.619.
[7]	F. Auricchio and L. Petrini, A three-dimensional model describing stress-temperature induced solid phase transformations. Part I: Solution algorithm and boundary value problems, Internat. J. Numer. Meth. Engrg., 61 (2004), 807-836. doi: 10.1002/nme.1086.
[8]	F. Auricchio and L. Petrini, A three-dimensional model describing stress-temperature induced solid phase transformations. Part II: Thermomechanical coupling and hybrid composite applications, Internat. J. Numer. Meth. Engrg., 61 (2004), 716-737. doi: 10.1002/nme.1087.
[9]	F. Auricchio, A. Reali and U. Stefanelli, A three-dimensional model describing stress-induces solid phase transformation with permanent inelasticity, Int. J. Plasticity, 23 (2007), 207-226. doi: 10.1016/j.ijplas.2006.02.012.
[10]	F. Auricchio, A. Reali and U. Stefanelli, A macroscopic 1D model for shape memory alloys including asymmetric behaviors and transformation-dependent elastic properties, Comput. Methods Appl. Mech. Engrg., 198 (2009), 1631-1637. doi: 10.1016/j.cma.2009.01.019.
[11]	N. Barrera, P. Biscari and M. F. Urbano, Macroscopic modeling of functional fatigue in shape memory alloys, Eur. J. Mech. A/Solids, submitted.
[12]	S. Bartels and T. Roubíček, Thermo-visco-elasticity with rate-independent plasticity in isotropic materials undergoing thermal expansion, Math. Modelling Numer. Anal., 45 (2011), 477-504. doi: 10.1051/m2an/2010063.
[13]	B. Benesova, M. Frost and P. Sedlak, A microscopically motivated constitutive model for shape memory alloys: formulation, analysis and computations, Preprint NCMM/2013/17, Necas center, Prague.
[14]	A.-L. Bessoud and U. Stefanelli, Magnetic shape memory alloys: Three-dimensional modeling and analysis, Math. Models Meth. Appl. Sci., 21 (2011), 1043-1069. doi: 10.1142/S0218202511005246.
[15]	A.-L. Bessoud, M. Kružík and U. Stefanelli, A macroscopic model for magnetic shape memory alloys, Preprint IMATI-CNR, 23PV10/21/0, 2010.
[16]	A. Berti, C. Giorgi and E. Vuk, Free energies and pseudo-elastic transitions for shape memory alloys, Discrete Cont. Dyn. S. - Series S, 6 (2013), 293-316.
[17]	V. Berti, M. Fabrizio and D. Grandi, Phase transitions in shape memory alloys: A non-isothermal Ginburg-Landau model, Physica D, 239 (2010), 95-102. doi: 10.1016/j.physd.2009.10.005.
[18]	H. Brézis, Operateurs Maximaux Monotones et Semi-Groupes de Contractions dans les Espaces de Hilbert, Math Studies, 5, North-Holland, Amsterdam/New York, 1973.
[19]	M. Brokate and J. Sprekels, Hysteresis and Phase Transitions, Applied Mathematical Sciences, 121, Springer-Verlag, New York, 1996. doi: 10.1007/978-1-4612-4048-8.
[20]	M. Brokate and J. Sprekels, Optimal control of shape memory alloys with solid-solid phase transitions, in Emerging applications in free boundary problems (Montreal, 1990), Pitman Res. Notes Math. Ser., 280, Longman Sci. Tech., Harlow, 1993, 208-214.
[21]	N. Bubner, J. Sokołowski and J. Sprekels, Optimal boundary control problems for shape memory alloys under state constraints for stress and temperature, Numer. Funct. Anal. Optim., 19 (1998), 489-498. doi: 10.1080/01630569808816840.
[22]	P. Colli and J. Sprekels, Global existence for a three-dimensional model for the thermodynamical evolution of shape memory alloys, Nonlinear Anal., 18 (1992), 873-888. doi: 10.1016/0362-546X(92)90228-7.
[23]	T. W. Duerig and A. R. Pelton editors, SMST-2003 Proceedings of the International Conference on Shape Memory and Superelastic Technology Conference, ASM International, 2003.
[24]	M. Eleuteri, J. Kopfová and P. Krejčí, A thermodynamic model for material fatigue under cyclic loading, Physica B: Condensed Matter, 407 (2012), 1415-1416. doi: 10.1016/j.physb.2011.10.017.
[25]	M. Eleuteri, J. Kopfová and P. Krejčí, Non-isothermal cyclic fatigue in an oscillating elastoplastic beam, Comm. Pure Appl. Anal., 12 (2013), 2973-2996. doi: 10.3934/cpaa.2013.12.2973.
[26]	M. Eleuteri, J. Kopfová and P. Krejčí, Fatigue accumulation in a thermo-visco-elastoplastic plate, Discrete Cont. Dyn. S. Series B, 19 (2014).
[27]	M. Eleuteri, L. Lussardi and U. Stefanelli, A rate-independent model for permanent inelastic effects in shape memory materials, Netw. Heterog. Media, 6 (2011), 145-165. doi: 10.3934/nhm.2011.6.145.
[28]	M. Eleuteri, L. Lussardi and U. Stefanelli, Thermal control of the Souza-Auricchio model for shape memory alloys, Discrete Cont. Dyn. S. - Series S, 6 (2013), 369-386.
[29]	V. Evangelista, S. Marfia and E. Sacco, Phenomenological 3D and 1D consistent models for shape-memory alloy materials, Comput. Mech., 44 (2009), 405-421. doi: 10.1007/s00466-009-0381-8.
[30]	V. Evangelista, S. Marfia and E. Sacco, A 3D SMA constitutive model in the framework of finite strain, Internat. J. Numer. Methods Engrg., 81 (2010), 761-785.
[31]	F. Falk, Martensitic domain boundaries in shape-memory alloys as solitary waves, J. Phys. C4 Suppl., 12 (1982), 3-15.
[32]	F. Falk and P. Konopka, Three-dimensional Landau theory describing the martensitic phase transformation of shape-memory alloys, J. Phys. Condens. Matter, 2 (1990), 61-77. doi: 10.1088/0953-8984/2/1/005.
[33]	M. Frémond, Matériaux à mémoire de forme, C. R. Acad. Sci. Paris Sér. II Méc. Phys. Chim. Sci. Univers Sci. Terre, 304 (1987), 239-244.
[34]	S. Frigeri and U. Stefanelli, Existence and time-discretization for the finite-strain Souza-Auricchio constitutive model for shape-memory alloys, Contin. Mech. Thermodyn., 24 (2012), 63-77. doi: 10.1007/s00161-011-0221-x.
[35]	K.-H. Hoffmann, M. Niezgódka and S. Zheng, Existence and uniqueness to an extended model of the dynamical developments in shape memory alloys, Nonlinear Anal., 15 (1990), 977-990. doi: 10.1016/0362-546X(90)90079-V.
[36]	K.-H. Hoffmann and D. Tiba, Control of a plate with nonlinear shape memory alloy reinforcements, Adv. Math. Sci. Appl., 7 (1997), 427-436.
[37]	K.-H. Hoffmann and A. Z. Ochowski, Control of the thermoelastic model of a plate activated by shape memory alloy reinforcements, Math. Methods Appl. Sci., 21 (1998), 589-603. doi: 10.1002/(SICI)1099-1476(19980510)21:7<589::AID-MMA904>3.0.CO;2-D.
[38]	O. Klein, Stability and uniqueness results for a numerical appproximation of the thermomechanical phase transitions in shape memory alloys, Adv. in Math. Sci. and Appl., 5 (1995), 91-116.
[39]	P. Krejčí and U. Stefanelli, Well-posedness of a thermo-mechanical model for shape memory alloys under tension, M2AN Math. Model. Numer. Anal., 44 (2010), 1239-1253. doi: 10.1051/m2an/2010024.
[40]	P. Krejčí and U. Stefanelli, Existence and nonexistence for the full thermomechanical Souza-Auricchio model of shape memory wires, Math. Mech. Solids, 16 (2011), 349-365. doi: 10.1177/1081286510386935.
[41]	G. A. Maugin, The Thermomechanics of Plasticity and Fracture, Cambridge Texts in Applied Mathematics. Cambridge University Press, Cambridge, 1992. doi: 10.1017/CBO9781139172400.
[42]	A. Mielke, Evolution of rate-independent systems, in Handbook of Differential Equations, Evolutionary Equations, (editors, C. Dafermos and E. Feireisl), 2 (2005), 461-559.
[43]	A. Mielke, L. Paoli and A. Petrov, On existence and approximation for a 3D model of thermally induced phase transformations in shape-memory alloys, SIAM J. Math. Anal., 41 (2009), 1388-1414. doi: 10.1137/080726215.
[44]	A. Mielke, L. Paoli, A. Petrov and U. Stefanelli, Error estimates for discretizations of a rate-independent variational inequality, SIAM J. Numer. Anal., 48 (2010), 1625-1646. doi: 10.1137/090750238.
[45]	A. Mielke and A. Petrov, Thermally driven phase transformation in shape-memory alloys, Adv. Math. Sci. Appl., 17 (2007), 667-685.
[46]	A. Mielke and F. Theil, On rate-independent hysteresis models, NoDEA, Nonlinear Diff. Equations Applications, 11 (2004), 151-189. doi: 10.1007/s00030-003-1052-7.
[47]	L. Paoli and A. Petrov, Global existence result for phase transformations with heat transfer in shape memory alloys, Preprint WIAS, 1608, (2011).
[48]	I. Pawłow, Three-dimensional model of thermomechanical evolution of shape memory materials, Control Cybernet., 29 (2000), 341-365.
[49]	F. Rindler, Optimal control for nonconvex rate-independent evolution processes, SIAM J. Control Optim., 47 (2008), 2773-2794. doi: 10.1137/080718711.
[50]	F. Rindler, Approximation of rate-independent optimal control problems, SIAM J. Numer. Anal., 47 (2009), 3884-3909. doi: 10.1137/080744050.
[51]	R. Rossi and M. Thomas, From an adhesive to a brittle delamination model in thermo-visco-elasticity, Quaderno 05/2012 del Seminario Matematico di Brescia, (2012), 1-50.
[52]	T. Roubíček, Thermodynamics of rate independent processes in viscous solids at small strains, SIAM J. Math. Anal., 42 (2010), 256-297. doi: 10.1137/080729992.
[53]	T. Roubíček and G. Tomassetti, Thermodynamics of shape-memory alloys under electric current, Zeit. angew. Math. Phys., 61 (2010), 1-20. doi: 10.1007/s00033-009-0007-1.
[54]	T. Roubíček and G. Tomassetti, Phase transformations in electrically conductive ferromagnetic shape-memory alloys, their thermodynamics and analysis, Arch. Rat. Mech. Anal., to appear. doi: 10.1007/s00205-013-0648-2.
[55]	A. Sadjadpour and K. Bhattacharya, A micromechanics-inspired constitutive model for shape-memory alloys, Smart Mater. Struct., 16 (2007), 1751-1765. doi: 10.1088/0964-1726/16/5/030.
[56]	J. Sokołowski and J. Sprekels, Control problems with state constraints for shape memory alloys, Math. Methods Appl. Sci., 17 (1994), 943-952. doi: 10.1002/mma.1670171204.
[57]	A. C. Souza, E. N. Mamiya and N. Zouain, Three-dimensional model for solids undergoing stress-induced tranformations, Eur. J. Mech. A/Solids, 17 (1998), 789-806. doi: 10.1016/S0997-7538(98)80005-3.
[58]	U. Stefanelli, Magnetic control of magnetic shape-memory single crystals, Phys. B, 407 (2012), 1316-1321. doi: 10.1016/j.physb.2011.06.043.
[59]	G. Wachsmuth, Optimal control of quasistatic plasticity with linear kinematic hardening, Part I: Existence and discretization in time, SIAM Journal on Control and Optimization (SICON), 50 (2012), 2836-2861. doi: 10.1137/110839187.
[60]	G. Wachsmuth, Optimal control of quasistatic plasticity with linear kinematic hardening, Part II: regularization and differentiability, Preprint SPP1253-119, 2011.
[61]	G. Wachsmuth, Optimal control of quasistatic plasticity with linear kinematic hardening, Part III: optimality conditions, Preprint SPP1253-119, 2011.
[62]	S. Yoshikawa, I. Pawłow and W. M. Zajączkowski, Quasi-linear thermoelasticity system arising in shape memory materials, SIAM J. Math. Anal., 38 (2007), 1733-1759. doi: 10.1137/060653159.

show all references

References:

[1]	T. Aiki and N. Kenmochi, Some models for shape memory alloys, Mathematical aspects of modelling structure formation phenomena, GAKUTO Internat. Ser. Math. Sci. Appl., Tokio, 17 (2002), 144-162.
[2]	M. Arndt, M. Griebel and T. Roubíček, Modelling and numerical simulation of martensitic transformation in shape memory alloys, Contin. Mech. Thermodyn., 15 (2003), 463-485. doi: 10.1007/s00161-003-0127-3.
[3]	F. Auricchio, A.-L. Bessoud, A. Reali and U. Stefanelli, A phenomenological model for the magneto-mechanical response of single-crystal magnetic shape memory alloys, Preprint IMATI-CNR 3PV13/3/0, 2013.
[4]	F. Auricchio, A.-L. Bessoud, A. Reali and U. Stefanelli, A three-dimensional phenomenological models for magnetic shape memory alloys, GAMM-Mitt., 34 (2011), 90-96. doi: 10.1002/gamm.201110014.
[5]	F. Auricchio, A. Mielke and U. Stefanelli, A rate-independent model for the isothermal quasi-static evolution of shape-memory materials, Math. Models Meth. Appl. Sci., 18 (2008), 125-164. doi: 10.1142/S0218202508002632.
[6]	F. Auricchio and L. Petrini, Improvements and algorithmical considerations on a recent three-dimensional model describing stress-induced solid phase transformations, Internat. J. Numer. Methods Engrg., 55 (2002), 1255-1284. doi: 10.1002/nme.619.
[7]	F. Auricchio and L. Petrini, A three-dimensional model describing stress-temperature induced solid phase transformations. Part I: Solution algorithm and boundary value problems, Internat. J. Numer. Meth. Engrg., 61 (2004), 807-836. doi: 10.1002/nme.1086.
[8]	F. Auricchio and L. Petrini, A three-dimensional model describing stress-temperature induced solid phase transformations. Part II: Thermomechanical coupling and hybrid composite applications, Internat. J. Numer. Meth. Engrg., 61 (2004), 716-737. doi: 10.1002/nme.1087.
[9]	F. Auricchio, A. Reali and U. Stefanelli, A three-dimensional model describing stress-induces solid phase transformation with permanent inelasticity, Int. J. Plasticity, 23 (2007), 207-226. doi: 10.1016/j.ijplas.2006.02.012.
[10]	F. Auricchio, A. Reali and U. Stefanelli, A macroscopic 1D model for shape memory alloys including asymmetric behaviors and transformation-dependent elastic properties, Comput. Methods Appl. Mech. Engrg., 198 (2009), 1631-1637. doi: 10.1016/j.cma.2009.01.019.
[11]	N. Barrera, P. Biscari and M. F. Urbano, Macroscopic modeling of functional fatigue in shape memory alloys, Eur. J. Mech. A/Solids, submitted.
[12]	S. Bartels and T. Roubíček, Thermo-visco-elasticity with rate-independent plasticity in isotropic materials undergoing thermal expansion, Math. Modelling Numer. Anal., 45 (2011), 477-504. doi: 10.1051/m2an/2010063.
[13]	B. Benesova, M. Frost and P. Sedlak, A microscopically motivated constitutive model for shape memory alloys: formulation, analysis and computations, Preprint NCMM/2013/17, Necas center, Prague.
[14]	A.-L. Bessoud and U. Stefanelli, Magnetic shape memory alloys: Three-dimensional modeling and analysis, Math. Models Meth. Appl. Sci., 21 (2011), 1043-1069. doi: 10.1142/S0218202511005246.
[15]	A.-L. Bessoud, M. Kružík and U. Stefanelli, A macroscopic model for magnetic shape memory alloys, Preprint IMATI-CNR, 23PV10/21/0, 2010.
[16]	A. Berti, C. Giorgi and E. Vuk, Free energies and pseudo-elastic transitions for shape memory alloys, Discrete Cont. Dyn. S. - Series S, 6 (2013), 293-316.
[17]	V. Berti, M. Fabrizio and D. Grandi, Phase transitions in shape memory alloys: A non-isothermal Ginburg-Landau model, Physica D, 239 (2010), 95-102. doi: 10.1016/j.physd.2009.10.005.
[18]	H. Brézis, Operateurs Maximaux Monotones et Semi-Groupes de Contractions dans les Espaces de Hilbert, Math Studies, 5, North-Holland, Amsterdam/New York, 1973.
[19]	M. Brokate and J. Sprekels, Hysteresis and Phase Transitions, Applied Mathematical Sciences, 121, Springer-Verlag, New York, 1996. doi: 10.1007/978-1-4612-4048-8.
[20]	M. Brokate and J. Sprekels, Optimal control of shape memory alloys with solid-solid phase transitions, in Emerging applications in free boundary problems (Montreal, 1990), Pitman Res. Notes Math. Ser., 280, Longman Sci. Tech., Harlow, 1993, 208-214.
[21]	N. Bubner, J. Sokołowski and J. Sprekels, Optimal boundary control problems for shape memory alloys under state constraints for stress and temperature, Numer. Funct. Anal. Optim., 19 (1998), 489-498. doi: 10.1080/01630569808816840.
[22]	P. Colli and J. Sprekels, Global existence for a three-dimensional model for the thermodynamical evolution of shape memory alloys, Nonlinear Anal., 18 (1992), 873-888. doi: 10.1016/0362-546X(92)90228-7.
[23]	T. W. Duerig and A. R. Pelton editors, SMST-2003 Proceedings of the International Conference on Shape Memory and Superelastic Technology Conference, ASM International, 2003.
[24]	M. Eleuteri, J. Kopfová and P. Krejčí, A thermodynamic model for material fatigue under cyclic loading, Physica B: Condensed Matter, 407 (2012), 1415-1416. doi: 10.1016/j.physb.2011.10.017.
[25]	M. Eleuteri, J. Kopfová and P. Krejčí, Non-isothermal cyclic fatigue in an oscillating elastoplastic beam, Comm. Pure Appl. Anal., 12 (2013), 2973-2996. doi: 10.3934/cpaa.2013.12.2973.
[26]	M. Eleuteri, J. Kopfová and P. Krejčí, Fatigue accumulation in a thermo-visco-elastoplastic plate, Discrete Cont. Dyn. S. Series B, 19 (2014).
[27]	M. Eleuteri, L. Lussardi and U. Stefanelli, A rate-independent model for permanent inelastic effects in shape memory materials, Netw. Heterog. Media, 6 (2011), 145-165. doi: 10.3934/nhm.2011.6.145.
[28]	M. Eleuteri, L. Lussardi and U. Stefanelli, Thermal control of the Souza-Auricchio model for shape memory alloys, Discrete Cont. Dyn. S. - Series S, 6 (2013), 369-386.
[29]	V. Evangelista, S. Marfia and E. Sacco, Phenomenological 3D and 1D consistent models for shape-memory alloy materials, Comput. Mech., 44 (2009), 405-421. doi: 10.1007/s00466-009-0381-8.
[30]	V. Evangelista, S. Marfia and E. Sacco, A 3D SMA constitutive model in the framework of finite strain, Internat. J. Numer. Methods Engrg., 81 (2010), 761-785.
[31]	F. Falk, Martensitic domain boundaries in shape-memory alloys as solitary waves, J. Phys. C4 Suppl., 12 (1982), 3-15.
[32]	F. Falk and P. Konopka, Three-dimensional Landau theory describing the martensitic phase transformation of shape-memory alloys, J. Phys. Condens. Matter, 2 (1990), 61-77. doi: 10.1088/0953-8984/2/1/005.
[33]	M. Frémond, Matériaux à mémoire de forme, C. R. Acad. Sci. Paris Sér. II Méc. Phys. Chim. Sci. Univers Sci. Terre, 304 (1987), 239-244.
[34]	S. Frigeri and U. Stefanelli, Existence and time-discretization for the finite-strain Souza-Auricchio constitutive model for shape-memory alloys, Contin. Mech. Thermodyn., 24 (2012), 63-77. doi: 10.1007/s00161-011-0221-x.
[35]	K.-H. Hoffmann, M. Niezgódka and S. Zheng, Existence and uniqueness to an extended model of the dynamical developments in shape memory alloys, Nonlinear Anal., 15 (1990), 977-990. doi: 10.1016/0362-546X(90)90079-V.
[36]	K.-H. Hoffmann and D. Tiba, Control of a plate with nonlinear shape memory alloy reinforcements, Adv. Math. Sci. Appl., 7 (1997), 427-436.
[37]	K.-H. Hoffmann and A. Z. Ochowski, Control of the thermoelastic model of a plate activated by shape memory alloy reinforcements, Math. Methods Appl. Sci., 21 (1998), 589-603. doi: 10.1002/(SICI)1099-1476(19980510)21:7<589::AID-MMA904>3.0.CO;2-D.
[38]	O. Klein, Stability and uniqueness results for a numerical appproximation of the thermomechanical phase transitions in shape memory alloys, Adv. in Math. Sci. and Appl., 5 (1995), 91-116.
[39]	P. Krejčí and U. Stefanelli, Well-posedness of a thermo-mechanical model for shape memory alloys under tension, M2AN Math. Model. Numer. Anal., 44 (2010), 1239-1253. doi: 10.1051/m2an/2010024.
[40]	P. Krejčí and U. Stefanelli, Existence and nonexistence for the full thermomechanical Souza-Auricchio model of shape memory wires, Math. Mech. Solids, 16 (2011), 349-365. doi: 10.1177/1081286510386935.
[41]	G. A. Maugin, The Thermomechanics of Plasticity and Fracture, Cambridge Texts in Applied Mathematics. Cambridge University Press, Cambridge, 1992. doi: 10.1017/CBO9781139172400.
[42]	A. Mielke, Evolution of rate-independent systems, in Handbook of Differential Equations, Evolutionary Equations, (editors, C. Dafermos and E. Feireisl), 2 (2005), 461-559.
[43]	A. Mielke, L. Paoli and A. Petrov, On existence and approximation for a 3D model of thermally induced phase transformations in shape-memory alloys, SIAM J. Math. Anal., 41 (2009), 1388-1414. doi: 10.1137/080726215.
[44]	A. Mielke, L. Paoli, A. Petrov and U. Stefanelli, Error estimates for discretizations of a rate-independent variational inequality, SIAM J. Numer. Anal., 48 (2010), 1625-1646. doi: 10.1137/090750238.
[45]	A. Mielke and A. Petrov, Thermally driven phase transformation in shape-memory alloys, Adv. Math. Sci. Appl., 17 (2007), 667-685.
[46]	A. Mielke and F. Theil, On rate-independent hysteresis models, NoDEA, Nonlinear Diff. Equations Applications, 11 (2004), 151-189. doi: 10.1007/s00030-003-1052-7.
[47]	L. Paoli and A. Petrov, Global existence result for phase transformations with heat transfer in shape memory alloys, Preprint WIAS, 1608, (2011).
[48]	I. Pawłow, Three-dimensional model of thermomechanical evolution of shape memory materials, Control Cybernet., 29 (2000), 341-365.
[49]	F. Rindler, Optimal control for nonconvex rate-independent evolution processes, SIAM J. Control Optim., 47 (2008), 2773-2794. doi: 10.1137/080718711.
[50]	F. Rindler, Approximation of rate-independent optimal control problems, SIAM J. Numer. Anal., 47 (2009), 3884-3909. doi: 10.1137/080744050.
[51]	R. Rossi and M. Thomas, From an adhesive to a brittle delamination model in thermo-visco-elasticity, Quaderno 05/2012 del Seminario Matematico di Brescia, (2012), 1-50.
[52]	T. Roubíček, Thermodynamics of rate independent processes in viscous solids at small strains, SIAM J. Math. Anal., 42 (2010), 256-297. doi: 10.1137/080729992.
[53]	T. Roubíček and G. Tomassetti, Thermodynamics of shape-memory alloys under electric current, Zeit. angew. Math. Phys., 61 (2010), 1-20. doi: 10.1007/s00033-009-0007-1.
[54]	T. Roubíček and G. Tomassetti, Phase transformations in electrically conductive ferromagnetic shape-memory alloys, their thermodynamics and analysis, Arch. Rat. Mech. Anal., to appear. doi: 10.1007/s00205-013-0648-2.
[55]	A. Sadjadpour and K. Bhattacharya, A micromechanics-inspired constitutive model for shape-memory alloys, Smart Mater. Struct., 16 (2007), 1751-1765. doi: 10.1088/0964-1726/16/5/030.
[56]	J. Sokołowski and J. Sprekels, Control problems with state constraints for shape memory alloys, Math. Methods Appl. Sci., 17 (1994), 943-952. doi: 10.1002/mma.1670171204.
[57]	A. C. Souza, E. N. Mamiya and N. Zouain, Three-dimensional model for solids undergoing stress-induced tranformations, Eur. J. Mech. A/Solids, 17 (1998), 789-806. doi: 10.1016/S0997-7538(98)80005-3.
[58]	U. Stefanelli, Magnetic control of magnetic shape-memory single crystals, Phys. B, 407 (2012), 1316-1321. doi: 10.1016/j.physb.2011.06.043.
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