Extended non‐linear relations of elastic shells undergoing phase transitions

The non-linear theory of elastic shells undergoing phase transitions was proposed by two first authors in J. Elast. 79, 67-86 (2004). In the present paper the theory is extended by taking into account also the elastic strain energy density of the curvilinear phase interface as well as the resultant forces and couples acting along the interface surface curve itself. All shell relations are found from the variational principle of stationary total potential energy. In particular, we derive the extended natural continuity conditions at coherent and/or incoherent surface curves modelling the phase interface. The continuity conditions allow one to establish the final position of the interface surface curve after the phase transition. The results are illustrated by an example of a phase transition in an infinite plate with a central hole.

[1]  Wojciech Pietraszkiewicz,et al.  The Nonlinear Theory of Elastic Shells with Phase Transitions , 2004 .

[2]  M. B. Rubin,et al.  A Cosserat shell model for interphases in elastic media , 2004 .

[3]  A. Boulbitch Equations of heterophase equilibrium of a biomembrane , 1999 .

[4]  Pavel A. Zhilin,et al.  Mechanics of deformable directed surfaces , 1976 .

[5]  Robert Finn,et al.  Equilibrium Capillary Surfaces , 1985 .

[6]  R. James,et al.  A theory of thin films of martensitic materials with applications to microactuators , 1999 .

[7]  A. Mielke,et al.  A Variational Formulation of¶Rate-Independent Phase Transformations¶Using an Extremum Principle , 2002 .

[8]  A. I. Rusanov,et al.  Surface thermodynamics revisited , 2005 .

[9]  Morton E. Gurtin,et al.  A continuum theory of elastic material surfaces , 1975 .

[10]  A. Roytburd,et al.  Coherent phase equilibria in a bending film , 2002 .

[11]  Ali Asghar Atai,et al.  Coupled Deformations of Elastic Curves and Surfaces , 1998, Recent Advances in the Mechanics of Structured Continua.

[12]  Y. Povstenko Generalizations of laplace and young equations involving couples , 1991 .

[13]  M. J. Grinfel'd,et al.  Thermodynamic methods in the theory of heterogeneous systems , 1991 .

[14]  J. G. Simmonds,et al.  The Nonlinear Theory of Elastic Shells , 1998 .

[15]  THERMODYNAMICS OF MOVING GIBBS DIVIDING SURFACES , 1997 .

[16]  Clifford Ambrose Truesdell,et al.  A first course in rational continuum mechanics , 1976 .

[17]  Pressurized Shape Memory Thin Films , 2000 .

[18]  W. Smoleński Statically and kinematically exact nonlinear theory of rods and its numerical verification , 1999 .

[19]  Morton E. Gurtin,et al.  Interface Evolution in Three Dimensions¶with Curvature-Dependent Energy¶and Surface Diffusion:¶Interface-Controlled Evolution, Phase Transitions, Epitaxial Growth of Elastic Films , 2002 .

[20]  E. Cosserat,et al.  Théorie des Corps déformables , 1909, Nature.

[21]  Robert V. Kohn,et al.  Elastic Energy Minimization and the Recoverable Strains of Polycrystalline Shape‐Memory Materials , 1997 .

[22]  Y. Shu,et al.  Heterogeneous Thin Films of Martensitic Materials , 2000 .

[23]  M. Gurtin,et al.  A Note on the Thermomechanics of Curvature Flows in IR3 and on Surfaces in IR3 , 1998 .

[24]  W. Pietraszkiewicz,et al.  Exact resultant equilibrium conditions in the non-linear theory of branching and self-intersecting shells , 2007 .

[25]  Witold Gutkowski,et al.  Mechanics of the 21st Century , 2005 .

[26]  A COORDINATE-FREE APPROACH TO SURFACE KINEMATICS , 1990 .