Series Solutions — Question 5

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Question 5

A formal power series is an algebraic coefficient expansion without an assumed positive radius of convergence. Investigate x2y‴−y″=−x,y(0)=y′(0)=y″(0)=0.x^2y'''-y''=-x,\qquad y(0)=y'(0)=y''(0)=0. For a possible one-sided smooth solution, you may use z(x)=∫0∞e−tx1−xtdt,x≤0.z(x)=\int_0^\infty e^{-t}\frac{x}{1-xt}\,dt,\qquad x\leq 0.

Tasks

  1. Put z=y″z=y'' and derive its formal coefficient recurrence. Find the first four nonzero terms of the formal series for yy.

  2. Prove that the formal series for yy has radius zero. Deduce whether an analytic solution at zero can satisfy the equation and data.

  3. Verify that the given integral defines a smooth function from the left at zero and satisfies x2z′−z=−xx^2z'-z=-x. Recover a one-sided smooth solution yy with the required initial data.

  4. Explain how this smooth solution can have the divergent formal series as its Taylor series. Identify the hypothesis that prevents application of the ordinary-point analytic existence theorem at zero.

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

Strategy. Separate formal coefficient solvability from convergence and from one-sided smooth existence.

Step 1: Compute the formal coefficients. For z=∑bnxnz=\sum b_nx^n, coefficient matching gives b0=0b_0=0, b1=1b_1=1, and bn=(n−1)bn−1b_n=(n-1)b_{n-1} for n≥2n\geq 2. Thus bn=(n−1)!b_n=(n-1)! for n≥1n\geq 1. Two integrations with zero constants give y∼∑n=1∞(n−1)!(n+1)(n+2)xn+2=x36+x412+x510+x65+⋯.\boxed{y\sim\sum_{n=1}^\infty\frac{(n-1)!}{(n+1)(n+2)}x^{n+2} =\frac{x^3}{6}+\frac{x^4}{12}+\frac{x^5}{10}+\frac{x^6}{5}+\cdots.}

Step 2: Prove divergence. The ratio of consecutive displayed coefficients is n(n+1)/(n+3)→∞n(n+1)/(n+3)\to\infty. For every fixed nonzero xx, the terms eventually fail to tend to zero. The radius is zero. Any analytic solution would have exactly these forced coefficients, so no analytic solution at zero exists.

Step 3: Construct and verify a smooth solution. For x≤0x\leq 0, 1−xt≥11-xt\geq 1. For n≥1n\geq 1, ∂xnx1−xt=n!tn−1(1−xt)n+1.\partial_x^n\frac{x}{1-xt}=\frac{n!t^{n-1}}{(1-xt)^{n+1}}. An integrable majorant permits differentiation of every order up to the left endpoint, giving z(0)=0z(0)=0 and z(n)(0−)=n!(n−1)!z^{(n)}(0-)=n!(n-1)!. Also x2z′−z=x∫0∞ddt(e−t1−xt)dt=−x.x^2z'-z=x\int_0^\infty\frac{d}{dt}\left(\frac{e^{-t}}{1-xt}\right)dt=-x. Hence y(x)=∫0x(x−v)z(v)dv\boxed{y(x)=\int_0^x(x-v)z(v)\,dv}, with oriented integration, is smooth on (−∞,0](-\infty,0], satisfies the equation there and has the zero initial triple. The equality at zero follows by continuity.

Step 4: Resolve the apparent contradiction. Its derivatives give exactly the formal coefficients above, but smoothness does not require the Taylor series to converge or represent the function. The leading coefficient x2x^2 vanishes at zero, so this is not an ordinary point. The analytic existence theorem for a normalized regular equation does not apply.

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

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