Fourier Sine Series — Question 2

PDF ↗

Question 2

Let f(x)=1f(x)=1 for 0<x<π0<x<\pi, with assigned endpoint values zero. The odd 2π2\pi-periodic extension is a square wave. Define its first MM nonzero modes by PM(x)=4π∑j=0M−1sin⁡((2j+1)x)2j+1.P_M(x)=\frac 4\pi\sum_{j=0}^{M-1}\frac{\sin((2j+1)x)}{2j+1}. You may use convergence to the average of the one-sided limits for piecewise smooth periodic functions.

Tasks

  1. Derive the sine coefficients and verify the definition of PMP_M. State the limiting values inside the interval and at its endpoints.

  2. Sum the finite cosine progression to prove PM′(x)=(2/π)sin⁡(2Mx)/sin⁡xP_M'(x)=(2/\pi)\sin(2Mx)/\sin x for 0<x<π0<x<\pi. Locate the first local maximum to the right of zero.

  3. Express the height of that maximum as an integral. Rescale the integral and prove that the heights tend to (2/π)∫0π(sin⁡t)/tdt(2/\pi)\int_0^\pi(\sin t)/t\,dt.

  4. Prove that this limiting height is greater than one, using sin⁡t/t≥1−t2/6\sin t/t\geq 1-t^2/6 for 0≤t≤π/20\leq t\leq\pi/2 and 1/t≥1/π1/t\geq 1/\pi for π/2≤t≤π\pi/2\leq t\leq\pi. Sketch P10P_{10} and explain why pointwise convergence does not remove the near-jump overshoot.

Original worksheet page 1: question and worked solution for 8-4-002
Show solutionHide solution

Question 2 – Solution

Strategy. Analyze a moving maximum of a finite sum rather than substitute a moving point into a pointwise convergence claim.

Step 1: Find the nonzero modes. Direct integration gives bn=2(1−(−1)n)/(πn)b_n=2(1-(-1)^n)/(\pi n): zero for even nn and 4/(πn)4/(\pi n) for odd nn. Thus PMP_M is the stated truncation. The odd extension has jump averages zero at both endpoints; its sum is one on (0,π)(0,\pi).

Step 2: Locate the first maximum. A finite geometric sum, or telescoping 2sin⁡xcos⁡((2j+1)x)2\sin x\cos((2j+1)x), gives ∑j=0M−1cos⁡((2j+1)x)=sin⁡(2Mx)/(2sin⁡x)\sum_{j=0}^{M-1}\cos((2j+1)x)=\sin(2Mx)/(2\sin x). Differentiating the finite sum is legitimate, so PM′(x)=2πsin⁡(2Mx)sin⁡x,xM=π2M.\boxed{P_M'(x)=\frac 2\pi\frac{\sin(2Mx)}{\sin x},\qquad x_M=\frac\pi{2M}.} The derivative is positive before xMx_M and negative just after it, for M≥1M\geq 1.

Step 3: Pass to the moving-peak limit correctly. Since PM(0)=0P_M(0)=0, substitution t=2Mxt=2Mx gives PM(xM)=2π∫0πsin⁡t2Msin⁡(t/(2M))dt→2π∫0πsin⁡ttdt.P_M(x_M)=\frac 2\pi\int_0^\pi \frac{\sin t}{2M\sin(t/(2M))}\,dt \longrightarrow\boxed{\frac 2\pi\int_0^\pi\frac{\sin t}{t}\,dt}. Write the integrand as (sin⁡t/t)(z/sin⁡z)(\sin t/t)(z/\sin z), where z=t/(2M)z=t/(2M). Since z/sin⁡zz/\sin z extends continuously with value one at zero, this factor tends uniformly to one for 0≤t≤π0\leq t\leq\pi. Also |sin⁡t/t|≤1|\sin t/t|\leq 1. These facts justify the integral limit; its value is approximately 1.1791.179.

Step 4: Prove a persistent excess. The supplied inequalities imply ∫0πsin⁡t/tdt≥π/2−π3/144+1/π>π/2\int_0^\pi\sin t/t\,dt\geq\pi/2-\pi^3/144+1/\pi>\pi/2, since π4<144\pi^4<144. The limiting peak is strictly above one. The peak location moves toward the jump, so convergence at each fixed interior point is consistent with this persistent overshoot. The square wave jumps by two across zero.

See the diagram in the original worksheet below.

Original worksheet page 2: question and worked solution for 8-4-002

Original worksheet layout. Use Enlarge or open the PDF for a closer view.