Instabilidades de Turing e Competição Aparente em Ambientes Fragmentados Marcus A.M. de Aguiar Lucas Fernandes IFGW - Unicamp Padrões de densidade em regiões homogêneas Vegetation in arid ecosystems Wolfram’s Cellular Automata After 250 iterations Complex Patterns can emerge out of simple interactions between neighboring cells on a homogeneous environment Cellular automata provide examples where direct interactions occur Another Mechanism: Reaction-Diffusion Systems and Turing Patterns 1912-1954 Summary 1. Turing Patterns in Homogeneous Environments 2. Turing Patterns in Networks of Fragments 3. Turing Patterns and Apparent Competition in Networks 1. Turing Patterns in Homogeneous Environments Reaction Populations of Preys (P) and Predators (Q) dP P PQ dt Lotka-Volterra Model dQ Q P Q dt ,,c and = constant coefficients The Mimura-Murray model On a diffusive prey-predator model which exhibits patchiness M. Mimura and J.D. Murray J. Ther. Biol. (1978) 75, 249-262 a bP P 2 Q P dt c dP dQ dt P (1 eQ ) Q a 35, b 16, c 9, e 2/5 Understanding the equation for the preys The growth rate per capta is 1 dP P dt a bP P 2 Q c logistic growth decrease because of predators Allee effect interspecies competition P Understanding the equation for the predators The growth rate per capta is 1 dQ (1 eQ ) P Q dt logistic growth Q increase because of preys mortality rate + interspecies competition Diffusion Add a new ingredient: space P(x,t) = population of preys at spatial position x at time t Q(x,t) = population of predators at spatial position x at time t Add a new interaction: migration The populations at x change by sending a fraction of its individuals to neighboring sites and receiving a fraction of individuals from the same sites. The math of diffusion k-1 k k+1 P(k-1) = 5 P(k) =7 P(k+1) = 8 P(k) – P(k-1) = 2 P (k ) P(k+1) – P(k) = 1 P ( k 1) P ( k ) P ( k ) P ( k 1) P ( k 1) P ( k 1) 2 P ( k ) A gradient in P(k) is not enough: diffusion requires a gradient of the gradient P 2 d x 2 back A uniform gradient is not enough k-1 k k+1 P(k-1) = 5 P(k) =7 P(k+1) = 9 P(k) – P(k-1) = 2 P (k ) P(k+1) – P(k) = 2 P ( k 1) P ( k ) P ( k ) P ( k 1) 0 The new equations describing the dynamics of Preys (P) and Predators (Q) become 2 a bP P 2 P Q P dP 2 t c x P diffusion local interactions Q t P (1 eQ ) Q Q 2 dQ x 2 diffusion coefficients Partial Differential Equations Can we understand these equations? Are there simple solutions? 1 - Look for solutions that are uniform in space, i.e., situations where the populations are the same at all points in space. In this case there is no diffusion! 2 2 P a bP P P Q P dP 2 t c x Q t P (1 eQ ) Q Q 2 dQ x 2 2 - Look for solutions that are constant in time: a bP P 2 Q P t c P Q t P (1 eQ ) Q Simplified equations can be solved: a bP P 2 Q P 0 c P (1 eQ ) Q a 35, b 16, c 9, 0 e 2/5 Two solutions: 1 – extinction Q=P=0 2 – coexistence Q0 = 10 P0 = 5. Are they stable? J. Theor. Biol. 1978 u=P=prey v=Q=pred Patterns of preys and predators emerging on a homogeneous environment. Preys distributed on patches. Predators everywhere, but with larger populations where the preys live. 2. Turing Patterns in Networks of Fragments Predator-Prey systems on a Network: Two main difficulties: 1 – describe diffusion in the network 2 – do the stability analysis Describe the network: 1 - labels the nodes from 1 to N in order of decreasing number of connections. 2 – Define the N x N adjancency matrix Aij = 1 if nodes i and j are connected Aij = 0 if nodes i and j are not connected 3 – ki = number of connections of node i Examples: 4 3 5 5 1 0 1 A 0 0 1 2 3 1 0 0 0 1 0 1 0 1 0 1 0 0 0 0 1 0 0 0 0 1 4 0 1 A 1 1 1 2 1 1 1 0 1 0 1 0 0 0 0 0 0 0 0 1 0 0 0 0 Model diffusion: Diffusion matrix Diffusion of u at node i L ij Aij k i ij N L N ij uj j 1 where ui is the population at node i ji Aij u j k i u i Example 1: 5 0 1 A 0 0 1 1 2 1 0 0 0 1 0 1 0 1 0 1 0 0 0 0 3 1 0 0 0 0 4 2 1 L 0 0 1 1 0 0 2 1 0 1 2 1 0 1 1 0 0 0 1 0 0 0 1 u1 u 2 u u3 u4 u 5 N For node 2: L 2 j u j u1 u 3 2 u 2 j 1 diffusion Example 2: 4 3 5 1 0 1 A 1 1 1 1 1 1 0 1 0 1 0 0 0 0 0 0 0 0 2 4 1 L 1 1 1 1 0 0 0 0 1 1 1 2 1 0 1 2 0 0 0 1 0 0 0 N For node 1: L 1j j 1 u j u 2 u 3 u 4 u 5 4 u1 1 0 0 0 1 u1 u 2 u u3 u4 u 5 New Notation: u = prey = P v = predator = Q N a bu i cu i 2 v i u i L ij u j dt c j 1 du i dv i dt N u i (1 dv i ) v i L ij v j each node is a fragment, a local community predator v j 1 For zero diffusion we are back to the same equations, for which there is a homogeneous solution: each community has the same number of preys and predators. We find ui = u0 = 5 and vi = v0 = 10 for all nodes prey u turn on diffusion: 0.12 15.6 Movies Hysteresis N A ( u i 1 i 2 2 u ) ( v i v ) 3. Turing Patterns and Apparent Competition in Networks N a bu i cu i 2 v i u i u i y i L ij u j dt c j 1 du i dv i dt N u i (1 dv i ) v i L ij v j j 1 N a bx i cx i 2 y i x i L ij x j dt c j 1 dx i predators v preys u dy i dt N x i (1 dy i ) y i f u i y i L ij y j j 1 y x Results Parameters: =0.12 =20.0 BA network with N=1000 Dynamics for first prey, u Dynamics for second prey, x Dynamics for u-x =0.05 f=0.5 Effect of Coupling Three nested predator-prey pairs in each node predators v y preys u x z Typical patterns: sites with v-u and z-w and low values of y-x sites with y-x and low values of v-u and z-w few sites with all species in equal proportions w Four predator-prey pairs in each node predators v y z r preys u x w s Typical patterns: sites with v-u and z-w and low values of y-x and r-s sites with y-x and r-s and low values of v-u and z-w few sites with all species in equal proportions Conclusions • on a homogeneous environment, density patterns can be generated dynamically, independent of intrinsic differences. • on a fragmented environment with identical patches, abundance distributions can be different: there will be two types of patches: with high abundance and with low abundance. • if more pairs of antagonistic species interact in each patch, strong effects of apparent competition can also be dinamically generated. There will be four types of patches: - high v and u with low y and x high y and x with low v and u low v, u, y and x. high v, u, y and x.