One of our research interests is to understand the microscopic origin of self-organization and macroscopic pattern formation in many-body systems out of equilibrium. This is the case of all systems in nature including biology at any level. The second law of thermodynamics does not allow self-organization and formation of spatial structures in thermal equilibrium because such processes in isolated systems reduces the entropy of the universe. Therefore, to form macroscopic spatial structures, the system must be open, interacting with the external world. In this case the system under consideration (a subsystem of the entire, isolated system) can self-organize and remain in this condition over time, reducing its entropy but increasing the total entropy of the universe. The requirement for the system being open is demanding and generates serious conceptual and practical problems: classical thermodynamics deals with equilibrium systems, and statistical mechanics concepts were developed to understand the microscopic origin of such thermodynamics. To deal with open systems it is first necessary to develop a non-equilibrium statistical mechanics theory to give microscopic basis to a non-equilibrium thermodynamics. These general theories are not trivial and sophisticated mathematical techniques and controversial concepts (e.g., how to deal with the problem of temporal irreversibility in nature) have to be dealt with. Physicists have already addressed this topic and some non-equilibrium approaches have been developed over the last decades. A particular approch is based on the Maximum Entropy formalism, which gives basis to a general non-equilibrium theory. The theory involves a generalization of the Gibbs and Boltzmann formulations combined with a variational principle, namely, the maximization of the information entropy. This is the general approach that connects the microscopic processes occuring in non-equilibrium systems with the macroscopic manifestation of such interactions. By definition, the thermodynamics arising out of this non-equilibrium statistical mechanics theory is the non-equilibrium thermodynamics mentioned above. Although still mathematically complex this macroscopic formalism leads to equations that can at least be solved numerically (read more). 

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