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The replicator dynamics derived from the last equation of (6c) with the matrix A is described by dx/dt = b x - a x2 - R x y dy/dt = -d y + f R x y This is in fact nothing but a good old Lotka-Volterra equationd of prey-predator type. We next introduce altruism into this game. Since the altruistic game matrix is given bythe transposed matrix A+ , a game plan specified by the mixture of egoism : altruism = κ : (1-κ) is decribed using a modified game matrix Aκ = κ A + (1-κ) A+ Replicator dynamics of this game matrix iscalculated as dx/dt = (1-κ)b x - a x2 - (1-κ- κf)R x y dy/dt = -(1-κ)d y + (f-κ- κf) R x y The satble fixed points of this set of differential equation vary with the value of k. By defining the quantity κ* = (f-ad/bR) / (1+f) we can classify them as follows. In case of κ > κ*, a stable fixed point is given by X = (1-κ)/(f-κ- κf)・(d/R) Y = (1-κ)/(1-κ- κf)・{ bR - ad/(f-κ- κf) }/R2 , while in case of κ < κ* , this point becomes unstable (namely, the neighboring linearized map becomes hyperbolic), and new stable point with extinct Y specified by X = (1-κ)b/a Y = 0 appears. We shall display this results graphically and give explanations. |
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t.cheon & associates
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