Real Eigenvalues — Question 5

Section 24-7 · Calculus pages 4389–4390

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Question 5

For a real parameter −1<a<1-1<a<1, consider X′=AaX,Aa=12(a−2a+2a+2a−2).X'=A_aX,\qquad A_a=\frac 12\begin{pmatrix}a-2&a+2\\a+2&a-2\end{pmatrix}. Treat the zero-eigenvalue case explicitly; do not assume that every equilibrium is isolated.

Tasks

  1. Find the eigenvalues, an eigenbasis independent of aa, and the solution with arbitrary initial state (p,q)T(p,q)^T.

  2. Classify the origin for a<0a<0 and a>0a>0, and identify the initial states that converge to it in each case.

  3. At a=0a=0, find every equilibrium and the limiting state of every solution. Is the origin attracting all nearby states?

  4. For initial state (2,0)T(2,0)^T, compare lim⁡a↑0lim⁡t→∞Xa(t)\lim_{a\uparrow 0}\lim_{t\to\infty}X_a(t) with lim⁡t→∞lim⁡a↑0Xa(t)\lim_{t\to\infty}\lim_{a\uparrow 0}X_a(t). Explain the difference.

Question 5 – Solution

Strategy. Keep the parameter-dependent mode visible; its decay disappears at the zero eigenvalue.

Step 1: Use fixed eigendirections. The vectors (1,1)T(1,1)^T and (1,−1)T(1,-1)^T have eigenvalues aa and −2-2. They remain independent, and their eigenvalues are distinct throughout the stated parameter interval. Setting m=(p+q)/2m=(p+q)/2, d=(p−q)/2d=(p-q)/2 gives Xa(t)=meat(11)+de−2t(1−1).\boxed{X_a(t)=m e^{at}\binom 11+d e^{-2t}\binom 1{-1}.} This formula satisfies the system and the initial data for every allowed aa.

Step 2: Classify the nonzero-parameter cases. For a<0a<0, both modes decay, so the origin is a stable node and all initial states converge to it. For a>0a>0, the origin is a saddle; convergence occurs exactly when m=0m=0, that is, on y=−xy=-x. The y=xy=x mode then grows. There are no other equilibria in these two cases because det⁡Aa=−2a≠0\det A_a=-2a\ne 0.

Step 3: Resolve the equilibrium line. At a=0a=0, every point on y=xy=x is an equilibrium and X0(t)→(m,m)TX_0(t)\to(m,m)^T. This is the orthogonal projection of the initial state onto that line. The origin does not attract all nearby states: nearby nonzero points of the equilibrium line remain fixed. Nevertheless it is stable in the distance sense, since the orthogonal constant and decaying modes never increase the Euclidean norm.

Step 4: Compare the orders of limiting. For the specified data, m=d=1m=d=1. At each fixed a<0a<0 the time limit is zero; hence the first iterated limit is (0,0)T\boxed{(0,0)^T}. At each fixed finite tt, taking a↑0a\uparrow 0 instead gives (1,1)T+e−2t(1,−1)T(1,1)^T+e^{-2t}(1,-1)^T, whose time limit is (1,1)T\boxed{(1,1)^T}. The decay eate^{at} becomes arbitrarily slow as aa approaches zero from below. It is not uniform over such parameters on an unbounded time interval, so these two operations need not commute.