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The need for functional forms is well known from equilibrium thermodynamics where, however, the functions of interest, that is, the thermodynamicpotentials, depend only on a few variables Beyond-equilibrium simulations involving many variables, even fields, thus pose a major challenge As a first possibility, we mention the most convenient situation that arises when the GENERIC building blocks on the target level are given functions with only a few free parameters, for example, obtained from some phenomenological model, experienced guessing, experimental results, or, more likely, from combinationsof all of those For this situation to occur, one needs a considerable a priori understanding of the problem of interest A second possibility is to determine the building blocks only for particular values of the independent variables z or, more frequently, for the corresponding Lagrange multipliers X (at least, for some of the variables).

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provided that condition (44.7) holds, i.e., (44.13) Now suppose that one more (block) row is added to H N - ~ one more (vector) entry is , added to $"-I, and one more invertible weighting block is added to W N - 1 leading to

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Rather than calculating SE(z)/Gz and SS(z)/Sz through differences, one should try to obtain these gradients directly For example, the relation (656) between entropy gradients and Lagrange multipliers shows how 6S(z)/6z can be obtained conveniently For such pointwise simulations, it is crucial to select a proper set of values of x or A Often, one is interested in a sequence of parameter values, in particular, as they are occurring in the course of time for some problem of interest If one is interested in steady states, for example, in steady homogeneous flows of complex fluids, one needs to estimate the Lagrange multipliers that lead to a generalized canonical ensemble of configurations characteristic of a given flow type and rate The choice of proper Lagrange multipliers to define a beyond-equilibrium ensemble again requires a priori information.

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0.047/ 0.174 0.104/ 0.375

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