Real Eigenvalues — Question 5

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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.

Original worksheet page 1: question and worked solution for 5-7-005
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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.

Original worksheet page 2: question and worked solution for 5-7-005

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