50 likes | 163 Vues
Explore linear stability at critical points of the model, including (0,0), (0,1), (1,0), and more. Learn how eigenvalues determine solution behavior and see detailed analysis with Jacobian matrices in LaTeX.
E N D
4 Critical Points • (0,0) • (0,1) • (1,0) • (n1 *,n2 *) • n1 * = (1-alpha2/beta)/ (1-alpha1alpha2) • n2 * = (1 – alpha1beta(1 – alpha2beta/(1- alpha1alpha2)))
Linear Stability • We notice that similar to a scalar ODE • dx/dt = Ax ,x(0) = x0 where denotes vector Has solution x(t) = x0 exp(At), where A is the Jacobian matrix
Decomposing A • By writing • A = SDS-1 • Exp(At) = exp[(SDS-1)t] • then taylor expanding the following • sum{ (SDS-1 t)n / n! } from 0…inf • we can see that the eigenvalues of A determine the behavior of the solution. • If Eig(A(criticalpt)) = both neg. then the point is stable • If Eig(A(criticalpt)) = both pos. then the point is unstable • If Eig(A(criticalpt)) = pos/ neg. then it is a saddle point
Tedious details of Analysis • This needs to be typed in latex • Show all A matrices evaluated at each critical point • Eigen values of each matrix A • Phase plane behavior determined by above. A couple plots for different cases of alphas, betas, etc. would be nice