Variation of Parameters — Question 3

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Question 3

On x>0x>0, consider the Euler-type equation x3y‴−3x2y″+6xy′−6y=x4ln⁡x.x^3y'''-3x^2y''+6xy'-6y=x^4\ln x. Use the proposed homogeneous basis x,x2,x3x,x^2,x^3 and variation of parameters, rather than a guessed logarithmic trial.

Tasks

  1. Verify the three homogeneous solutions and their Wronskian. Normalize the equation and write the parameter system with the correct right-hand side.

  2. Solve for the parameter derivatives and integrate to obtain one particular solution. Write the complete general solution.

  3. Impose y(1)=y′(1)=y″(1)=0y(1)=y'(1)=y''(1)=0. Verify all three initial data and the forcing directly.

  4. State the interval containing 11 on which this construction and the standard linear IVP theorem apply. Explain why evaluating the same parameter system at x=0x=0 is invalid, even if some expressions have finite limits there.

Original worksheet page 1: question and worked solution for 7-4-003
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Question 3 – Solution

Strategy. Normalize the Euler operator before solving the derivative equations, and retain its positive-domain restriction.

Step 1: Verify the basis and normalization. For y=xmy=x^m, the left side is (m−1)(m−2)(m−3)xm(m-1)(m-2)(m-3)x^m. Thus the proposed functions are homogeneous. Their Wronskian is 2x3≠02x^3\ne 0 for x>0x>0. Division by x3x^3 gives normalized forcing xln⁡xx\ln x, so (xx2x312x3x2026x)(u1′u2′u3′)=(00xln⁡x).\begin{pmatrix}x&x^2&x^3\\1&2x&3x^2\\0&2&6x\end{pmatrix} \begin{pmatrix}u_1'\\u_2'\\u_3'\end{pmatrix} =\begin{pmatrix}0\\0\\x\ln x\end{pmatrix}.

Step 2: Integrate the solved parameter derivatives. Elimination gives u1′=x2ln⁡x/2u_1'=x^2\ln x/2, u2′=−xln⁡xu_2'=-x\ln x, u3′=ln⁡x/2u_3'=\ln x/2. Convenient antiderivatives are u1=x3ln⁡x6−x318,u2=−x2ln⁡x2+x24,u3=xln⁡x2−x2.u_1=\frac{x^3\ln x}{6}-\frac{x^3}{18},\quad u_2=-\frac{x^2\ln x}{2}+\frac{x^2}{4},\quad u_3=\frac{x\ln x}{2}-\frac{x}{2}. Combining xu1+x2u2+x3u3xu_1+x^2u_2+x^3u_3 gives yp=x4(ln⁡x6−1136),y=yp+c1x+c2x2+c3x3.\boxed{y_p=x^4\left(\frac{\ln x}{6}-\frac{11}{36}\right),\qquad y=y_p+c_1x+c_2x^2+c_3x^3.} Integration constants are already represented by the homogeneous terms.

Step 3: Fit and check the initial vector. The particular solution has vector (−11/36,−19/18,−5/2)(-11/36,-19/18,-5/2) at 11. The three linear equations for its cancellation give y=x18−x24+x32+x4(ln⁡x6−1136).\boxed{y=\frac{x}{18}-\frac{x^2}{4}+\frac{x^3}{2} +x^4\left(\frac{\ln x}{6}-\frac{11}{36}\right).} The added terms have vector (11/36,19/18,5/2)(11/36,19/18,5/2), verifying the data. For a direct residual check, let θ=xD\theta=xD. The operator is (θ−1)(θ−2)(θ−3)(\theta-1)(\theta-2)(\theta-3); on x4(aln⁡x+b)x^4(a\ln x+b) it gives x4(6aln⁡x+11a+6b)x^4(6a\ln x+11a+6b). With a=1/6,b=−11/36a=1/6,b=-11/36, this is exactly x4ln⁡xx^4\ln x.

Step 4: Respect the regular interval. The normalized coefficients, forcing and nonsingular derivative matrix are valid throughout (0,∞)(0,\infty), the largest such interval containing 11. At zero the leading coefficient and Wronskian vanish and ln⁡x\ln x is undefined. Finite limits of selected terms do not make that parameter system invertible or extend the theorem across zero.

Original worksheet page 2: question and worked solution for 7-4-003

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