Convergence of Fourier Series — Question 5

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Question 5

Consider H(x)=∑n=1∞sin⁡nxn3.H(x)=\sum_{n=1}^{\infty}\frac{\sin nx}{n^3}. You may use the theorem: if a series of C1C^1 functions converges at one point and its derivative series converges uniformly, its sum is C1C^1 and may be differentiated term by term. Also use ∑n=1∞cos⁡nxn2=π26−πx2+x24,0≤x≤2π.\sum_{n=1}^{\infty}\frac{\cos nx}{n^2} =\frac{\pi^2}{6}-\frac{\pi x}{2}+\frac{x^2}{4},\qquad 0\leq x\leq 2\pi.

Tasks

  1. Verify every hypothesis needed to differentiate the series once on [0,2π][0,2\pi].

  2. Integrate the given derivative formula to obtain a closed form for HH. Check the endpoint values and slopes of its periodic extension.

  3. Determine whether the periodic extension is C2C^2. Identify precisely where the formal second derivative series agrees with the classical second derivative.

  4. Prove that the second derivative partial sums cannot converge uniformly to the interior second derivative on (0,2π)(0,2\pi). Explain why the first differentiation remains valid.

Original worksheet page 1: question and worked solution for 8-7-005
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Question 5 – Solution

Strategy. Check a separate convergence condition for each differentiation; one valid differentiation does not authorize the next.

Step 1: Justify the first differentiation. Every summand is C1C^1. The original series converges at 00 (all terms are zero), and the derivative terms satisfy |cos⁡nx/n2|≤1/n2|\cos nx/n^2|\leq 1/n^2. The Weierstrass test gives uniform convergence of the derivative series. The stated theorem therefore gives H′(x)=∑n=1∞cos⁡nxn2.\boxed{H'(x)=\sum_{n=1}^{\infty}\frac{\cos nx}{n^2}.} This includes one-sided endpoint derivatives on the closed interval.

Step 2: Verify the explicit function. Integrating the provided formula and using H(0)=0H(0)=0 gives H(x)=π2x6−πx24+x312,0≤x≤2π.\boxed{H(x)=\frac{\pi^2x}{6}-\frac{\pi x^2}{4}+\frac{x^3}{12}, \qquad 0\leq x\leq 2\pi.} Both endpoint values are zero. Both endpoint slopes equal π2/6\pi^2/6, so the periodic extension is C1C^1 across the join.

Step 3: Identify the second derivative obstruction. Inside the period, H″(x)=−π/2+x/2H''(x)=-\pi/2+x/2. Its right limit at zero is −π/2-\pi/2, whereas its left periodic limit is π/2\pi/2. Thus the periodic function is not twice differentiable at the join and is not C2C^2. The formal second derivative series is −∑sin⁡(nx)/n-\sum\sin(nx)/n. The piecewise smooth Fourier theorem, or direct coefficients of the displayed linear function, gives H″H'' on 0<x<2π0<x<2\pi. At a join the series equals zero, the average of the limits, where the classical periodic second derivative does not exist.

Step 4: Rule out uniform second differentiation. Every finite sum −∑n=1Nsin⁡(nx)/n-\sum_{n=1}^N\sin(nx)/n tends to zero as x↓0x\downarrow 0, but the interior target tends to −π/2-\pi/2. Thus its error supremum on the full open period is at least π/2\pi/2 for every NN. The derivative series for the first differentiation had summable bounds n−2n^{-2}; the next series has no such global uniform convergence. There is no contradiction between a valid first differentiation and failure of the stronger second-derivative conclusion.

Original worksheet page 2: question and worked solution for 8-7-005

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