Repeated Roots — Question 7

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Question 7

Consider the parameter family y″+2y′+(1−μ)y=0,y(0)=0,y′(0)=1,−1<μ<1.y''+2y'+(1-\mu)y=0,\qquad y(0)=0,\qquad y'(0)=1, \qquad -1<\mu<1. For convenience, sinh⁡z=(ez−e−z)/2\sinh z=(e^z-e^{-z})/2. You may use sin⁡z/z→1\sin z/z\to 1 and sinh⁡z/z→1\sinh z/z\to 1 as z→0z\to 0.

Tasks

  1. Solve the IVP separately for μ>0\mu>0, μ=0\mu=0 and μ<0\mu<0, identifying the root type in each case.

  2. Prove that the formulas from both sides tend to the repeated-root solution for each fixed t≥0t\ge 0 as μ→0\mu\to 0.

  3. Determine which of these solutions have positive-time zeros. For μ<0\mu<0, find the first positive zero and its limit as μ↑0\mu\uparrow 0.

  4. Prove that every solution of every equation in the stated parameter range tends to zero as t→∞t\to\infty. Explain why convergence of the displayed IVP solutions on any fixed time window does not preserve their number of positive-time zeros.

Original worksheet page 1: question and worked solution for 3-4-007
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Question 7 – Solution

Strategy. Center the characteristic equation at its repeated root and compare the resulting real, repeated and complex formulas without conflating their global zero patterns.

Step 1: Solve each root case. The characteristic polynomial is (r+1)2−μ(r+1)^2-\mu. If μ>0\mu>0, set s=μ∈(0,1)s=\sqrt\mu\in(0,1). The roots are −1±s-1\pm s and the data give yμ=e−tsinh⁡(st)s.y_\mu=e^{-t}\frac{\sinh(st)}s. At μ=0\mu=0, the root is −1-1 twice, and the solution is y0=te−t\boxed{y_0=te^{-t}}. If μ<0\mu<0, set b=−μ>0b=\sqrt{-\mu}>0; the roots are −1±ib-1\pm ib, giving yμ=e−tsin⁡(bt)b.y_\mu=e^{-t}\frac{\sin(bt)}b. Each formula has value 0 and derivative 1 at zero and solves its stated equation.

Step 2: Recover the repeated-root limit from either side. For t>0t>0, factor the first formula as te−tsinh⁡(st)/(st)te^{-t}\sinh(st)/(st) and the third as te−tsin⁡(bt)/(bt)te^{-t}\sin(bt)/(bt). The supplied limits yield yμ(t)→te−ty_\mu(t)\to te^{-t} from either side. At t=0t=0, all values are zero directly. Thus the repeated-root solution is the common fixed-time limit, rather than a missing special value.

Step 3: Locate zeros before taking their limit. For μ≥0\mu\ge 0, the displayed solution is strictly positive for every t>0t>0, since t>0t>0 and sinh⁡(st)>0\sinh(st)>0. For μ<0\mu<0, its positive zeros are tn=nπ−μ,n=1,2,….\boxed{t_n=\frac{n\pi}{\sqrt{-\mu}},\qquad n=1,2,\ldots}. In particular, t1→∞t_1\to\infty as μ↑0\mu\uparrow 0. The infinitely many oscillations move beyond every fixed finite observation window.

Step 4: Separate decay from zero counts. For 0<μ<10<\mu<1, both roots −1±μ-1\pm\sqrt\mu are negative; at zero, both repeated-root modes decay; for μ<0\mu<0, the exponential factor e−te^{-t} bounds every fixed sine/cosine combination. Hence every solution decays throughout the stated parameter range.

On any fixed [0,T][0,T], the ratios in Step 2 converge uniformly because their arguments lie in intervals shrinking to zero and both ratios extend continuously with value 1 there. Yet for every negative μ\mu there are infinitely many later zeros, while y0y_0 has none for t>0t>0. Convergence on fixed windows does not control zeros that escape to infinity.

Original worksheet page 2: question and worked solution for 3-4-007

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