Geometric stability analysis

For the phase stability analysis we follow the method given by Kanamori and Kakehashi of geometrical inequalities and compute the antiphase boundary energy defined by... 

Computational techniques are centrally important at every stage of investigation of nonlinear dynamical systems. We have reviewed the main theoretical and computational tools used in studying these problems among these are bifurcation and stability analysis, numerical techniques for the solution of ordinary differential equations and partial differential equations, continuation methods, coupled lattice and cellular automata methods for the simulation of spatiotemporal phenomena, geometric representations of phase space attractors, and the numerical analysis of experimental data through the reconstruction of phase portraits, including the calculation of correlation dimensions and Lyapunov exponents from the data. 

An elastic stability analysis is presented in this paper for Timoshenko-type beams with variable cross sections taking into consideration the effects of shear deformations under the geometrically non-linear theory based on large displacements and rotations. The constitutive relationship for stresses and finite strains based on a consistent finite strain hyperelastic formulation is proposed. The generalized equilibrium equations for varying arbitrary cross-sectional beams are developed from the virtual work equation. The second variation of the Total Potentid is also derived which enables... 

These fascinating bicontinuous or sponge phases have attracted considerable theoretical interest. Percolation theory [112] is an important component of such models as it can be used to describe conductivity and other physical properties of microemulsions. Topological analysis [113] and geometric models [114] are useful, as are thermodynamic analyses [115-118] balancing curvature elasticity and entropy. Similar elastic modulus considerations enter into models of the properties and stability of droplet phases [119-121] and phase behavior of microemulsions in general [97, 122]. 

The extended Brusselator [2, 5], Oregonator [5, 10] and other similar systems [4, 7] demonstrate other autowave processes whose distinctive spatial and temporal properties are independent on initial concentrations, boundary conditions and often even on geometrical size of a system. As it was noted by Zhabotinsky [4], Vasiliev, Romanovsky and Yakhno [5], a number of well-documented results obtained in the theory of autowave processes is much less than a number of problems to be solved. In fact, mathematical methods for analytical solution of the autowave equations and for analysis of their stability are practically absent so far. 

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