C2 FUNDAMENTAL THEORY OF DYNAMICAL SYSTEMS EXAMPLE SHEET 4 Stars indicate difficulty of questions. 1. Let Γ be a periodic orbit of a differential equation on Rn of period T. Let Σ be a Poincaré section and g the corresponding return map. Let x*∈Σ ∩ Γ be the corresponding fixed points of g. Show that if the linearization MT around the orbit has an eigenvalue λ = 1 of multiplicity k, then D x*g has an eigenvalue λ = 1 of multiplicity k-1. Similarly, show that if MT has an eigenvalue λ ≠ 1 of multiplicity k, then the same holds for Dx*g. Make sure that you take due consideration of the possibility of non-trivial Jordan Normal Forms. 2. Suppose that A = P -1BP. Show that a) det (A) = det (B) b) the eigenvalues of A are the same as those of B. 3. Show that trace (BA) = trace (AB) for any two matrices A and B. 4. Let A be a n×n matrix with an eigenvalue λ of multiplicity n. Suppose that A has only one linearly independent eigenvector v1, and v2, …, vn are generalized eigenvectors obtained by solving (A - λI)v2 = v1 M (A - λI)vi = vi-1 M (A - λI)vn = vn-1 with vi ≠ 0 for i = 2, …, n. Let P = [v 1, v2, …, vn] be the matrix whose columns are v 1, v2, …, vn. Show that P -1AP = B, where B is the n×n Jordan block B 5. = λ 0 M 0 0 1 0 K λ 1 L M O M 0 L λ 0 L 0 0 0 M 1 λ Find an example of two matrices A and B such that e Ate Bt ≠ e (A+B)t 6. Show that e Ate -At = Id for any matrix A. 7. Show that e At = Id if A = 0. C2 Exercise Sheet 4 8. Consider the linear differential equation d dt x y λ 0 = 1 λ x y Show that x(t) satisfies d -λt (e x(t)) dt = y(0) and hence that x(t) = e λt(x(0) + y(0)t) Use this to compute expBt where B 9. = λ 0 1 λ Recall that in Q12, Ex. Sheet 1, you solved the linear differential equation d x dt y x B y = using polar co-ordinates, where B = a b −b a Use this to compute expBt. 10. Compute expBt by direct summation of the series, where B = λ 0 1 λ Hint: consider the expression for Bn derived in lectures. 11. Compute expBt by direct summation of the series, where B = a b −b a Hint: consider ∞ ∑ n! λ 1 n (cos nϕ + i sin nϕ)tn n=0 where a = λcos ϕ and b = λsin ϕ. 12. C2 May 1994 Q2i) and ii) 2