Stano Pekár“Populační ekologie živočichů“ dN = Nr dt Acarus Cheyletus continuous model of Lotka & Volterra (1925-1928) used to explain decrease in prey fish and increase in predatory fish after World War I assumptions - continuous predation (high population density) - populations are well mixed - closed populations (no immigration or emigration) - no stochastic events - predators are specialised on one prey species - populations are unstructured - reproduction immediately follows feeding H .. density of prey P .. density of predators r .. intrinsic rate of prey population m .. predator mortality rate a .. predation rate b .. reproduction rate of predators in the absence of predator, prey grows exponentially → in the absence of prey, predator dies exponentially → predation rate is linear function of the number of prey .. aHP each prey contributes identically to the growth of predator .. bHP rH t H = d d mP t P −= d d aHPrH t H −= d d mPbHP t P −= d d do not converge, has no asymptotic stability (trajectories are closed lines) → neutral stability unstable system, amplitude of the cycles is determined by initial numbers Zero isoclines: for prey population: for predator population: H P prey isocline predator isocline 0 0 d d = t P aHPrH −=0 a r P = mPbHP −=0 b m H = 0 d d = t H timedensity prey predator 0 Analysis of the model a r b m in the absence of the predator prey population reaches carrying capacity K Addition of density-dependence for given parameter values: r = 3, m = 2, a = 0.1, b = 0.3, K = 10 HP H H t H 1.0 10 13 d d −      −= PHP t P 23.0 d d −= aHP K H rH t H −      −= 1 d d mPbHP t P −= d d Zero isoclines: for prey population: if H = 0 (trivial solution) or if for predator population: 0.3HP - 2P = 0 if P = 0 (trivial solution) or if 0.3H - 2 = 0 gradient of prey isocline is negative 0 d d = t H HP H H 1.0 10 130 −      −= 0 d d = t P P = 30 - 3H P H 1.0 10 130 −      −= H = 6.667 H P 30 6.670 10 time density prey predator 0 K H P 30 6.70 10 has single positive asymptotically stable equilibrium defined by crossing of isoclines converges to the stable equilibrium functional response Type II: rate of consumption by all predators: Addition of functional response of Type II for parameters: rH = 3, a = 0.1, Th = 2, K = 10 prey isocline: predator isocline: h a aHT aHT H + = 1 h a aHT aHP T PH + = 1 h H aHT aHP K H Hr t H + −      −= 1 1 d d 0 d d = t H 21.01 1.0 10 130 H HPH H + −      −= 2 6.0630 HHP −+= mPbHP t dP −= d H = constant .. damped oscillations predator exploits prey close to K - isocline: H = 9 time density time density time density predator exploits prey close to K/2 - isocline: H = 5 predator exploits prey at low density - isocline: H = 2 Rosenzweig & MacArthur (1963) H P H P H P K prey predator 0 0 0 0 0 0K/2 K Damped oscillations Sustained oscillations Extinction K K logistic model with carrying capacity proportional to H k .. carrying capacity of the predator rP = bH - m Addition of predator’s carrying capacity for parameters: rP = 2, k = 0.2 predator isocline: prey isocline: mPbHP t P −= d d       −= kH P Pr t P P 1 d d 0 d d = t P       −= H P P 2.0 120 H = 5P 2 6.0630 HHP −+= h H aHT aHP K H Hr t H + −      −= 1 1 d d H P K0 time density prey predator 0 K H P K0 quick approach to stable equilibrium Zatypota Theridion discrete model of Nicholson & Bailey (1935) - discrete generations - 1, .., several, or less than 1 host - random host search and functional response Type III - lay eggs in aggregation Ht = number of hosts in time t Ha = number of attacked hosts λ = finite rate of increase of the host Pt = number of parasitoids c = conversion rate, no. of parasitoids for 1 host )(1 att HHH −=+ λ aat HcHP ==+1 parasitoid searches randomly encounters (x) are random (Poisson distribution) p0 = proportion of not encountered, µ .. mean number of encounters Et = total number of encounters a = searching efficiency (proportion of hosts encountered) Et = a Ht Pt proportion of encounters (1 or more times): p = (1– p0) Incorporation of random search x = 0, 1, 2, ... !x e p x x µ µ − = µ− = ep0 ( )taP ta eHH − −= 1 t t t aP H E ==µ taP ep − =0 )1( taP ep − −= highly unstable model for all parameter values: - equilibrium is possible but the slightest disturbance leads to divergent oscillations (extinction of parasitoid) taP tt eHH − + = λ1 ( )taP tt eHP − + −= 11 time density H P 0 0 )(1 att HHH −=+ λ at HP =+1 exponential growth of hosts is replaced by logistic equation H*.. new host carrying capacity depends on parasitoids’ efficiency - when a is low then q → 1 - when a is high then q → 0 density-dependence have stabilising effect for moderate r and q Stability boundaries Addition of density-dependence Beddington et al. (1975) t t aP K H tt eHH −      − + = 1 1 λ ( )taP tt eHP − + −= 11 K H q * = Addition of the refuge if hosts are distributed non-randomly in the space Fixed number in refuge: H0 hosts are always protected have strong stabilising effect even for large r Hassell & May (1973) taP tt eHHHH − + −+= )( 001 λλ ( )taP tt eHHP − + −−= 1)( 01 distribution of encounters is not random but aggregated (negative binomial distribution) - proportion of hosts not encountered (p0): where k = degree of aggregation very stable model system if k ≤ 1 Stability boundaries: a) k=∝, b) k=2, c) k=1, d) k=0 Addition of aggregated distribution Hassell (1978) k tt k aP K H tt eHH −       +      − + = 11 1 λ               +−= − + k t tt k aP HP 111 k t k aP p −       += 10