Euler Equations — Question 8

PDF ↗

Question 8

For fixed a∈ℝa\in\mathbb R and parameter ε≥0\varepsilon\ge 0, consider on x>0x>0 x2y″+(1−2a)xy′+(a2−ε2)y=0.x^2y''+(1-2a)xy'+(a^2-\varepsilon^2)y=0. Two distinct power solutions become nearly identical when their characteristic exponents approach one another.

Tasks

  1. Find the characteristic exponents for ε>0\varepsilon>0 and explain why simply taking their two power solutions to the limit does not produce a fundamental pair at ε=0\varepsilon=0.

  2. Construct solutions uε,vεu_\varepsilon,v_\varepsilon satisfying uε(1)=1u_\varepsilon(1)=1, uε′(1)=au_\varepsilon'(1)=a, vε(1)=0v_\varepsilon(1)=0, vε′(1)=1v_\varepsilon'(1)=1.

  3. Compute their Wronskian and prove independence for every ε≥0\varepsilon\ge 0, using the limiting pair at zero.

  4. Determine that limiting pair and justify uniform convergence of each basis function on every compact interval [r,R]⊂(0,∞)[r,R]\subset(0,\infty) as ε→0\varepsilon\to 0. Explain how the logarithmic repeated-root solution emerges.

Original worksheet page 1: question and worked solution for 6-4-008
Show solutionHide solution

Question 8 – Solution

Strategy. Normalize a symmetric sum and a divided difference before allowing the characteristic roots to merge.

Step 1: Identify the degenerating pair. The power equation is (m−a)2−ε2=0(m-a)^2-\varepsilon^2=0, giving m=a±εm=a\pm\varepsilon. Both xa+εx^{a+\varepsilon} and xa−εx^{a-\varepsilon} tend to xax^a as ε→0\varepsilon\to 0. Their separate limits are the same function, so they cannot remain a fundamental pair.

Step 2: Normalize before taking the limit. For ε>0\varepsilon>0, set t=ln⁡xt=\ln x and define uε=xacosh⁡(εt),vε=xasinh⁡(εt)ε.\boxed{u_\varepsilon=x^a\cosh(\varepsilon t),\qquad v_\varepsilon=x^a\frac{\sinh(\varepsilon t)}{\varepsilon}.} These are the half-sum and the difference divided by 2ε2\varepsilon of the two powers. At x=1x=1 they have the four required value/slope data by direct differentiation.

Step 3: Check the determinant exactly. Differentiation and cosh⁡2s−sinh⁡2s=1\cosh^2s-\sinh^2s=1 give W(uε,vε)=x2a−1>0.\boxed{W(u_\varepsilon,v_\varepsilon)=x^{2a-1}>0.} At ε=0\varepsilon=0, define u0=xau_0=x^a and v0=xaln⁡xv_0=x^a\ln x. They solve the repeated-root equation, have the same normalized data, and their Wronskian is again x2a−1x^{2a-1}. Independence holds for every parameter value.

Step 4: Justify the limit uniformly. On [r,R][r,R], let T=max⁡(|ln⁡r|,|ln⁡R|)T=\max(|\ln r|,|\ln R|) and M=max⁡[r,R]xaM=\max_{[r,R]}x^a. For 0<ε≤10<\varepsilon\le 1, Taylor’s theorem for cosh\cosh and sinh\sinh gives |uε−u0|≤Mε2T2cosh⁡T2,|vε−v0|≤Mε2T3cosh⁡T6.|u_\varepsilon-u_0|\le\frac{M\varepsilon^2T^2\cosh T}{2},\qquad |v_\varepsilon-v_0|\le\frac{M\varepsilon^2T^3\cosh T}{6}. Both bounds tend to zero uniformly. The divided difference tends to ∂mxm|m=a=xaln⁡x\partial_m x^m|_{m=a}=x^a\ln x, recovering the independent logarithmic solution that the two unnormalized limits lose.

Original worksheet page 2: question and worked solution for 6-4-008

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