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4 Chemotactic Cell Motion and Biological Pattern Formation
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                              of production/decay is a multiple of a constant γ which depends on the ‘size’ of
                              the modeling domain B. To complete the model, we assume that we know the
                              concentrations of the chemicals at time t = 0

                                                 u(., t = 0) = u I  and v(., t = 0) = v I        (4.7)
                              and that, starting from the initial point in time, the two chemicals can neither
                              flow out of the domain B, nor is any of the two chemicals added. In mathematical
                              terms we express this by the homogeneous Neumann boundary conditions

                                                 ν · grad u = ν · grad v = 0on ∂B ,              (4.8)

                              where ∂B is the boundary of the domain B and ν is the unit outward normal
                              vector to this boundary. Note that the formulation of production/decay using the
                              two functions f (u, v)and g(u, v) allows that both chemicals may influence their
                              ownproduction/decayaswellasproduction/decayoftheotherone.Nevertheless
                              fromnowonweshallinterpretthechemicalwithconcentrationuastheactivator,
                              i.e. it is likely to increase morphogen production, whereas we shall interpret
                              the chemical associated to the concentration v as the deactivator. Hence the
                              presence of the latter chemical is likely to reduce production or even stimulates
                              consumption of the morphogen.
                                 The central idea of Turing instability is to construct systems of chemicals
                              with the following property: The concentrations of the chemicals are linearly
                              stable if they are homogeneous. Clearly, variations of concentrations necessarily
                              lead to diffusive effects. If the diffusion coefficients are different (i.e. d  = 1), then
                              diffusion shall lead to instability (“diffusion driven instability”) in the sense that
                              initial variations in concentrations get amplified.
                                 This was a novel concept since in the mathematical field of partial differential
                              equations (PDEs) diffusion is usually considered to be a stabilising process, just
                              like variations in temperature in general get equilibrated and inhomogeneous
                              concentrations are expected to smooth out.
                                 The mechanism which in the present case leads to instability works as fol-
                              lows: Imagine regions where, for whatever reason, there is a high concentration
                              of activators and where, as a consequence of activation, lots of inhibitors are pro-
                              duced. The Turing mechanism is based on the fact that the inhibitor substance
                              diffuses faster than the activator chemical. So in these regions the deactivators
                              will diffuse away quickly and will not be able to reduce the concentration of
                              activators.
                                 Most notably in situations, where the size of the modeling domain is finite
                              and where chemicals can neither leave nor enter the domain, the inhibitors



                              Fig. 4.5. Zebra coat pattern
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