Series Solutions — Question 10

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Question 10

For ε>0\varepsilon>0, consider the fourth-order initial-value problem εy(4)+y″=0,(y,y′,y″,y‴)(0)=(0,0,1,0).\varepsilon y^{(4)}+y''=0,\qquad (y,y',y'',y''')(0)=(0,0,1,0). A Taylor approximation accurate for each fixed parameter need not be accurate uniformly as the parameter tends to zero.

Tasks

  1. Derive the Taylor recurrence, sum the solution series, and determine its radius for each fixed ε>0\varepsilon>0.

  2. Prove uniform convergence of yεy_\varepsilon and yε′y_\varepsilon' on the whole real line as ε↓0\varepsilon\downarrow 0. Show that yε″y_\varepsilon'' has no limit at any fixed nonzero xx.

  3. At fixed x≠0x\ne 0, investigate the limit of every fixed even-degree Taylor truncation of degree at least two. Explain why taking a parameter limit and truncating the series give incompatible conclusions.

  4. Use ξ=x/ε\xi=x/\sqrt\varepsilon to obtain a parameter-independent profile. Give a uniform Taylor error bound for bounded ξ\xi, and plot the profile and its degree-six polynomial on 0≤ξ≤π0\leq\xi\leq\pi.

Original worksheet page 1: question and worked solution for 7-7-010
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Question 10 – Solution

Strategy. Resolve the shrinking oscillation scale before judging a series truncation.

Step 1: Derive and sum the series. The recurrence is an+4=−an+2/[ε(n+4)(n+3)]a_{n+4}=-a_{n+2}/[\varepsilon(n+4)(n+3)], with a0=a1=a3=0a_0=a_1=a_3=0, a2=1/2a_2=1/2. Therefore yε=∑j=1∞(−1)j+1x2j(2j)!εj−1=ε(1−cos⁡(x/ε)).\boxed{y_\varepsilon=\sum_{j=1}^\infty \frac{(-1)^{j+1}x^{2j}}{(2j)!\varepsilon^{j-1}} =\varepsilon\bigl(1-\cos(x/\sqrt\varepsilon)\bigr).} The radius is infinite for each fixed positive parameter. The formula verifies all four initial derivatives and the equation directly.

Step 2: Distinguish levels of derivative convergence. The bounds |yε|≤2ε|y_\varepsilon|\leq 2\varepsilon and |yε′|≤ε|y_\varepsilon'|\leq\sqrt\varepsilon prove uniform convergence to zero on ℝ\mathbb R. But yε″=cos⁡(x/ε)y_\varepsilon''=\cos(x/\sqrt\varepsilon). For fixed x≠0x\ne 0, the sequences εn=x2/(2πn)2\varepsilon_n=x^2/(2\pi n)^2 and ε̃n=x2/((2n+1)π)2\widetilde\varepsilon_n=x^2/((2n+1)\pi)^2 give values 11 and −1-1. No pointwise limit exists there. The reduced equation y″=0y''=0 cannot retain the original second-derivative datum.

Step 3: Test fixed truncations. The degree-two polynomial is x2/2x^2/2, which fails to approach zero at fixed nonzero xx. For any fixed degree 2m≥42m\geq 4, its highest term is a nonzero constant times ε1−m\varepsilon^{1-m} and dominates the lower powers as ε↓0\varepsilon\downarrow 0. Thus the truncation diverges while the full sum tends to zero. The Taylor remainder is not uniform in this parameter at fixed xx.

Step 4: Rescale and certify. With yε/ε=1−cos⁡ξy_\varepsilon/\varepsilon=1-\cos\xi, Taylor’s theorem gives, for |ξ|≤R|\xi|\leq R, |1−cosξ−∑j=1m(−1)j+1ξ2j(2j)!|≤R2m+2(2m+2)!.\left|1-\cos\xi-\sum_{j=1}^m\frac{(-1)^{j+1}\xi^{2j}}{(2j)!}\right| \leq\frac{R^{2m+2}}{(2m+2)!}. Multiplying by ε\varepsilon bounds the original displacement error. For the graph, m=3m=3, R=πR=\pi, so the profile error is at most π8/40320\pi^8/40320.

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Original worksheet page 2: question and worked solution for 7-7-010

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