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Tamtam Proceedings - lamsin

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A topology Nash game 293. The Nash gameWe consider a two-players static game of complete information. The two players arethe Tumoral Angiogenic Factors (TAF) which control activators distribution, denoted byµ, and anti-Angiogenic Factors (aAF) which control inhibitors distribution, denoted by k.Strategy spaces are defined as follows :– (TAF) is equipped with a strategy spaceS 1 = {µ ∈ L ∞ (Ω), 0 ≤ µ ≤ 1,– (aAF) is equipped with a strategy spaceS 2 = {k ∈ L ∞ (Ω), 0 ≤ k ≤ 1,∫∫ΩΩµdx ≤ γ 1 |Ω|}kdx ≤ γ 2 |Ω|}The constraints on the relative volume fractions express the fact that there is only a limitedavailable amount of activators and inhibitors.A simultaneous (or blind) choice of (µ; k) prompts an interaction between TAF andaAF, which is modeled as follows :– Interaction Law : θ = µ(1 − k)– Porosity : ρ = ρ (µ; k) = ρ M + (ρ V − ρ M )P (θ)– Elasticity tensor : E = E (µ; k) = E M + (E D − E M )P (θ)where P (θ) is the identity, an exact homogenization operator, or an interpolated SIMPlike(Solid Isotropic Material Penalization) operator, see Rozvany et al. [10].The interaction law is a very simple, arbitrary, choice. It states for example that theinhibitor action is completely and immediately efficient. Actual biological situations areof course much more complex.To end with the definition of the game, objective or loss functions are defined respectivelyas :Pressure Drop j 1 (µ; k) = L 1 (ρ; p) for player (TAF) (3)Mechanical Compliance j 2 (µ; k) = L 2 (E; u) for player (aAF) (4)where p is the pressure solution to the D’Arcy equation (1), and u is the displacementvector solution to the elasticity equation (2).3.1. Existence of a Nash equilibriumWe consider the cases where either P (θ) = θ or P (θ) is a restriction operator,i.e. P (θ) = g ◦ S R (θ), with g being a convex function and S R a linear compact filter,cf [2] for details. We have theTAMTAM –Tunis– 2005

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