Fourier Cosine Series — Question 3

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Question 3

Consider the normalized Neumann problem −u″=x−π/2,u′(0)=u′(π)=0,∫0πu(x)dx=0.-u''=x-\pi/2,\qquad u'(0)=u'(\pi)=0,\qquad \int_0^\pi u(x)dx=0. Use the convention u=a0/2+∑n≥1ancos⁡nxu=a_0/2+\sum_{n\geq 1}a_n\cos nx.

Tasks

  1. Derive the integral compatibility condition for a general forcing ff with these derivative conditions. Explain why replacing the forcing by xx makes the problem impossible.

  2. Find the cosine coefficients of the stated forcing. Explain how the zero mode differs from every positive-frequency mode when solving for uu.

  3. Solve in closed form and as a cosine series. Verify the equation, both derivative conditions and the mean.

  4. Prove uniqueness with the normalization, and state the full family without it. Explain why adding a constant cannot repair an incompatible forcing.

Original worksheet page 1: question and worked solution for 8-5-003
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Question 3 – Solution

Strategy. Check the forcing mean before dividing by eigenvalues; the constant mode has eigenvalue zero.

Step 1: Check compatibility before solving. Integration gives ∫0πf=−u′(π)+u′(0)=0\int_0^\pi f=-u'(\pi)+u'(0)=0. The stated forcing satisfies this condition, whereas ∫0πx=π2/2≠0\int_0^\pi x=\pi^2/2\ne 0. The replacement is impossible regardless of the additive level of uu.

Step 2: Solve the mode equations. The forcing has mean zero and coefficients Fn=2((−1)n−1)/(πn2)F_n=2((-1)^n-1)/(\pi n^2). Since −(cos⁡nx)″=n2cos⁡nx-(\cos nx)''=n^2\cos nx, an=2((−1)n−1)πn4(n≥1).\boxed{a_n=\frac{2((-1)^n-1)}{\pi n^4}\quad(n\geq 1).} The zero-mode equation is 0=00=0 and leaves the mean free. The normalization sets a0=0a_0=0; dividing this equation by zero would be invalid.

Step 3: Verify an independent polynomial solution. Direct integration gives u=−x36+πx24−π324=−4π∑j=0∞cos⁡((2j+1)x)(2j+1)4.\boxed{u=-\frac{x^3}{6}+\frac{\pi x^2}{4}-\frac{\pi^3}{24} =-\frac 4\pi\sum_{j=0}^\infty\frac{\cos((2j+1)x)}{(2j+1)^4}.} Its derivative is x(π−x)/2x(\pi-x)/2, zero at both ends, and −u″=x−π/2-u''=x-\pi/2. The mean of the first two terms is π3/24\pi^3/24, canceled by the constant. Twice integrating its coefficient integral by parts using u′=0u'=0 at the endpoints gives n2an=Fnn^2a_n=F_n, verifying the coefficients. The continuous piecewise smooth even extension identifies the series sum.

Step 4: Separate the free constant from compatibility. A difference satisfies w″=0w''=0 and zero endpoint derivatives, hence is constant. Its zero mean forces it to vanish. Without normalization, all solutions are the displayed polynomial plus any real constant. Adding a constant changes neither the equation nor its derivative conditions, so it cannot fix the integrated forcing balance.

Original worksheet page 2: question and worked solution for 8-5-003

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