Matrix Exponentials, Hyperbolic Fixed Points, Dulac's Negative Criterion and Lyapunov Functions Flashcards
What type of equations does the matrix exponential method solve?
-linear differential systems with constant coefficients
Taylor Series of an Exponential Function in 1D
e^(at) = 1 + at + 1/2! at² + 1/3! at³ + …
Taylor Series of an Exponential Function of a Matrix
exp(At) = I + At + 1/2! A²t² + 1/3! A³t³ + …
- where A is an nxn matrix and I is the identity matrix
- this series always converges and can be computed in a closed form
Proposition:
Let A be a square matrix with constant entries…
…then:
i) the exponential matrix X(t)=exp(At) satisfies the differential equation X’=AX
ii) any solution X(t) of the differential equation X’=AX satisfying the initial condition X(0)=I is given by X(t)=exp(At)
iii) solution of the initial value problem |x’=A|x, |x(0)=|xo is given by |x(t) = exp(At)*|xo
Properties of Matrix Exponentials
1) exp(0A) = I
2) if AB=BA, then:
exp(A)exp(B) = exp(A+B) = exp(B)exp(A)
3) if A = UBU^(-1) then, exp(UBU^(-1)) = Uexp(B)U^(-1)
4) if A is 2x2 matrix with first row α, 0 and second row 0,β, then exp(A) is a 2x2 matrix with entries first row: e^α, 0 and second row: 0, e^β
What are the two cases for the matrix exponential method?
Case a -> λ1≠λ2
Case b -> λ1=λ2
Case B: λ1=λ2
Solution
-let (2x22) matrix A have eigenvalues λ1=λ2, then:
exp(At) = e^(λ1t) * (I + t(A-λ1I))
Proposition
λ1=λ2
-let A be a 2x2 matrix with such that λ1=λ2 (i.e. eigenvalues coincide)
-then:
(A-λ1I)² = |0
-this is also true for nxn matrices with coninciding eigenvalues:
(A-λ1I)^n = 0
Nilpotent
Definition
-a matrix B such that B^n = |0 for some n∈ℕ is called a nilpotent matrix
Case B) λ1=λ2
Proof
A = A - λ1I + λ1I
-let B = A - λ1I
A = B + λ1I
-since I commutes with any matrix, [B,λ1I]=0, B and λ1I commute
exp(At) = exp(Bt + λ1It) = exp(Bt)exp(λ1It)
-expand the exponentials using the Taylor series:
exp(Bt) = I + Bt + B²t²/2! + …., by B²=0 by the λ1=λ2 proposition
exp(Bt) = I + Bt + 0 + 0 + … = I + Bt
exp(λ1It) = exp(2x2) with entries tλ1, 0, 0, tλ1
= exp(2x2) with entries e^(tλ1), 0, 0, e^(tλ1) = e^(tλ1)I
-sub back in:
exp(At) = (I + Bt) (e^(tλ1)I)
= e^(tλ1)(I + Bt)
= e^(tλ1)(I + t(A-λ1I))
Case A) λ1≠λ2
Solution
exp(At) = U(2x2)U^(-1)
-where the 2x2 has entries e^(tλ1), 0, 0, e^(tλ2)
Case A) λ1≠λ2
Proof
-consider 2x2 matrix A with eigenvalues λ1, λ2 such that λ1≠λ2
-has eigenvalues |v1, |v2 which will be linearly independent since λ1≠λ2
-let U=(|v1, |v2)
AU = A(|v1,|v2) = (A|v1, A|v2) = (λ1|v1,λ2|v2) = (|v1,|v2)(2x2)
-where 2x2 has entries, λ1, 0, 0, λ2, so:
AU = U(2x2)
AUU^(-1) = A = U(2x2)U^(-1)
-take exponential:
exp(At) = exp(U(2x2)U^(-1)) where 2x2 now has entries tλ1, 0, 0, tλ2
exp(At) = exp(U(2x2)U^(-1)) = Uexp(2x2))U^(-1)
exp(At) = U(2x2)U^(-1)
-where (2x2) now has entries e^(tλ1), 0, 0, e^(tλ2)
Behaviour at Hyperbolic vs Non-Hyperbolic Fixed Points
- at a non-hyperbolic point a small peterbation of the system can completely change the nature stability of the fixed poin
- at a hyperbolic fixed point this doesn’t happen
Hyperbolic Fixed Point
Linear System Definition
- a fixed point at the origin of the linear system |x’=A|x is hyperbolic if each eigenvalue of A has non-zero real part
- otherwise it is called a non-hyperbolic fixed point
Hyperbolic Fixed Point
Non-Linear System Definition
-a fixed point |x* of a non-linear system is hyperbolic if it is hyperbolic for the corresponding linearised system