Euler Equations — Question 2

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Question 2

For x>0x>0, consider x2y″−3xy′+4y=0,y(1)=1,y′(1)=3.x^2y''-3xy'+4y=0,\qquad y(1)=1,\quad y'(1)=3. A repeated characteristic exponent needs a second independent solution and careful treatment at the singular point.

Tasks

  1. Derive the repeated exponent and obtain a second independent solution using logarithmic coordinates. Verify independence rather than merely listing two functions.

  2. Solve the IVP and find every positive zero of its solution.

  3. Determine whether this IVP solution admits a continuous, C1C^1, or C2C^2 extension to 00. Compute the relevant one-sided limits.

  4. For the general positive-half-line solution, classify which choices permit a C2C^2 extension through 00 that solves the original equation. Explain whether the data y(0)=y′(0)=0y(0)=y'(0)=0 determine that extension uniquely.

Original worksheet page 1: question and worked solution for 6-4-002
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Question 2 – Solution

Strategy. A repeated exponential in logarithmic time produces a logarithmic factor in the original variable.

Step 1: Construct a genuine fundamental pair. With t=ln⁡xt=\ln x, the equation becomes Y″−4Y′+4Y=0Y''-4Y'+4Y=0, whose characteristic polynomial is (m−2)2(m-2)^2. Thus y=x2(A+Bln⁡x).y=x^2(A+B\ln x). For u=x2u=x^2, v=x2ln⁡xv=x^2\ln x, the Wronskian is W=x2(2xln⁡x+x)−2x(x2ln⁡x)=x3≠0W=x^2(2x\ln x+x)-2x(x^2\ln x)=x^3\ne 0 on x>0x>0.

Step 2: Use both initial values. At 11, y(1)=Ay(1)=A and y′(1)=2A+By'(1)=2A+B. Hence A=B=1A=B=1, giving y=x2(1+ln⁡x).\boxed{y=x^2(1+\ln x).} Because x2>0x^2>0, the only positive zero is x=e−1\boxed{x=e^{-1}}.

Step 3: Test successive derivatives at zero. For this solution, y′=x(3+2ln⁡x),y″=5+2ln⁡x.y'=x(3+2\ln x),\qquad y''=5+2\ln x. As x→0+x\to 0^+, y→0y\to 0 and y′→0y'\to 0, but y″→−∞y''\to-\infty. Defining y(0)=0y(0)=0 gives a right-hand C1C^1 extension with derivative 00: indeed y(x)/x=x(1+ln⁡x)→0y(x)/x=x(1+\ln x)\to 0. It can be joined to zero on the negative side as a C1C^1 function, but no C2C^2 extension is possible.

Step 4: Classify classical extensions. In general, y″=2A+B(2ln⁡x+3)y''=2A+B(2\ln x+3), so a finite second-derivative limit requires B=0B=0. On x<0x<0 the general solution is x2(C+Dln⁡|x|)x^2(C+D\ln|x|). A C2C^2 join similarly forces D=0D=0, and matching second derivatives forces C=AC=A. Thus precisely y=Ax2\boxed{y=Ax^2} extend through 00 as C2C^2 solutions of the original equation. Each satisfies y(0)=y′(0)=0y(0)=y'(0)=0, so these data do not give uniqueness at the singular point.

Original worksheet page 2: question and worked solution for 6-4-002

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