Convergence of Fourier Series — Question 7

PDF ↗

Question 7

For real bounded piecewise continuous 2π2\pi-periodic ff, its degree-one Fourier projection is (S1f)(x)=12π∫−ππf(x−t)(1+2cos⁡t)dt.(S_1f)(x)=\frac 1{2\pi}\int_{-\pi}^{\pi}f(x-t)(1+2\cos t)\,dt. Use the essential supremum norm, which ignores changes on sets of measure zero.

Tasks

  1. Prove ∥S1f∥∞≤Λ∥f∥∞\|S_1f\|_\infty\leq\Lambda\|f\|_\infty, where Λ=(2π)−1∫−ππ|1+2cos⁡t|dt\Lambda=(2\pi)^{-1}\int_{-\pi}^{\pi}|1+2\cos t|\,dt.

  2. Compute Λ\Lambda exactly, locating every sign change of the kernel.

  3. Construct an admissible ff with ∥f∥∞=1\|f\|_\infty=1 for which equality is attained at x=0x=0. Verify its mean and first cosine coefficient directly.

  4. Use the result to give a sharp worst-case amplification factor for a bounded input error under S1S_1. Explain why orthogonal projection being a contraction in L2L^2 does not imply contraction in the supremum norm.

Original worksheet page 1: question and worked solution for 8-7-007
Show solutionHide solution

Question 7 – Solution

Strategy. The signed Fourier kernel controls integral projection, while its absolute integral controls worst-case pointwise error.

Step 1: Bound the projection in the supremum norm. Taking absolute values in the given integral gives |S1f(x)|≤∥f∥∞2π∫−ππ|1+2cos⁡t|dt.|S_1f(x)|\leq\frac{\|f\|_\infty}{2\pi} \int_{-\pi}^{\pi}|1+2\cos t|\,dt. Null-set changes do not affect this estimate or the projected polynomial. Taking the supremum over xx proves the claimed inequality.

Step 2: Integrate the absolute kernel. The kernel is nonnegative for |t|≤2π/3|t|\leq 2\pi/3 and negative outside. Its full signed integral is 2π2\pi. Its integral on the two negative intervals is 2∫2π/3π(1+2cos⁡t)dt=2π3−23.2\int_{2\pi/3}^{\pi}(1+2\cos t)\,dt=\frac{2\pi}{3}-2\sqrt 3. Changing the sign of that contribution gives Λ=13+23π>1.\boxed{\Lambda=\frac 13+\frac{2\sqrt 3}{\pi}>1.}

Step 3: Attain the bound with an explicit input. Choose f(t)=sgn⁡(1+2cos⁡t)f(t)=\operatorname{sgn}(1+2\cos t), with value zero at its two zeros. It is even and piecewise constant with essential supremum one. Its positive region has length 4π/34\pi/3, so its mean is 1/31/3. Direct integration gives a1=2π(∫02π/3costdt−∫2π/3πcostdt)=23π,b1=0.a_1=\frac 2\pi\left(\int_0^{2\pi/3}\cos t\,dt -\int_{2\pi/3}^{\pi}\cos t\,dt\right)=\frac{2\sqrt 3}{\pi},\qquad b_1=0. Hence S1f(0)=1/3+23/π=ΛS_1f(0)=1/3+2\sqrt 3/\pi=\Lambda, proving sharpness.

Step 4: Interpret the stability statement. For input error ee with ∥e∥∞≤ε\|e\|_\infty\leq\varepsilon, linearity gives ∥S1(f+e)−S1f∥∞≤Λε\|S_1(f+e)-S_1f\|_\infty\leq\Lambda\varepsilon. The choice e=εsgn⁡(1+2cos⁡t)e=\varepsilon\operatorname{sgn}(1+2\cos t) attains this bound. Orthogonal projection still satisfies ∥S1e∥2≤∥e∥2\|S_1e\|_2\leq\|e\|_2 by the Pythagorean identity. That statement uses an integral norm, and does not prevent a larger pointwise peak. Contraction is a property of a specified norm.

Original worksheet page 2: question and worked solution for 8-7-007

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