Basic Concepts for nth Order Linear Equations — Question 7

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Question 7

Consider the singular third-order equation xy‴−2y″=0xy'''-2y''=0 on the whole real line. A classical solution here means a C3C^3 function satisfying the original equation at every point, including 00.

Tasks

  1. Solve on each half-line by first setting z=y″z=y''. Display all constants before matching across zero.

  2. Classify every global C3C^3 solution and determine the dimension of this solution space.

  3. For prescribed y(0)=αy(0)=\alpha, y′(0)=βy'(0)=\beta, y″(0)=γy''(0)=\gamma, determine exactly when solutions exist and how many free parameters remain.

  4. Determine which global solutions are C4C^4. Does demanding this extra derivative restore uniqueness for compatible initial data at zero? Explain why the regular third-order dimension theorem cannot be used across this singular point.

Original worksheet page 1: question and worked solution for 7-1-007
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Question 7 – Solution

Strategy. Solve separately where the leading coefficient is nonzero, then impose the actual regularity required at the join.

Step 1: Solve on both regular components. For x≠0x\ne 0, xz′−2z=0xz'-2z=0 gives z=Cx2z=Cx^2. Two integrations, with the constant absorbed into the quartic coefficient, yield y={A+x4+B+x+C+,x>0,A−x4+B−x+C−,x<0.y=\begin{cases}A_+x^4+B_+x+C_+,&x>0,\\ A_-x^4+B_-x+C_-,&x<0. \end{cases} The constants on the two components are initially independent.

Step 2: Impose a classical join. Continuity of yy and y′y' forces C+=C−=CC_+=C_-=C and B+=B−=BB_+=B_-=B. The second and third derivatives are 12A±x212A_\pm x^2 and 24A±x24A_\pm x, both tending to zero, so C3C^3 regularity imposes no relation between A+A_+ and A−A_-. Every global solution is therefore y(x)=C+Bx+{A+x4,x≥0,A−x4,x<0,\boxed{y(x)=C+Bx+\begin{cases}A_+x^4,&x\ge 0,\\A_-x^4,&x<0,\end{cases}} with four independent constants. At zero the equation reduces to −2y″(0)=0-2y''(0)=0, which these functions satisfy. This is a four-dimensional solution space.

Step 3: Classify the initial data. Every solution has y(0)=Cy(0)=C, y′(0)=By'(0)=B and y″(0)=0y''(0)=0. Thus γ=0\boxed{\gamma=0} is necessary and sufficient. When it holds, C=αC=\alpha, B=βB=\beta and both A+,A−A_+,A_- remain arbitrary. When γ≠0\gamma\ne 0, no classical solution exists.

Step 4: Check the extra derivative. The one-sided fourth derivatives are 24A+24A_+ and 24A−24A_-. A C4C^4 join requires and is guaranteed by A+=A−=AA_+=A_-=A, giving the polynomial C+Bx+Ax4C+Bx+Ax^4. One free parameter AA still survives for the compatible initial data, so uniqueness is not restored. The leading coefficient vanishes at 00, and normalization introduces −2/x-2/x. The hypotheses guaranteeing dimension three and arbitrary unique initial data hold only on the separate half-lines.

Original worksheet page 2: question and worked solution for 7-1-007

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