Series Solutions — Question 8

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Question 8

An unknown equation has the form y″+αxy′+(β+γx2)y=0,y''+\alpha x y'+(\beta+\gamma x^2)y=0, where α,β,γ\alpha,\beta,\gamma are real constants. Two analytic solutions have measured Taylor expansions u(x)=1−x2+12x4−16x6+O(x8),v(x)=x−x3+12x5−16x7+O(x9).u(x)=1-x^2+\tfrac 12x^4-\tfrac 16x^6+O(x^8),\qquad v(x)=x-x^3+\tfrac 12x^5-\tfrac 16x^7+O(x^9). The displayed coefficients are exact.

Tasks

  1. Determine α,β,γ\alpha,\beta,\gamma by substituting only the coefficients needed from these data. Show the recovery is unique.

  2. Derive the full recurrence for a generic series solution of the recovered equation, including its conventions at the lowest indices.

  3. Use the substitution y=e−x2wy=e^{-x^2}w to identify every solution exactly. Verify that the two measured series are a fundamental pair and determine their radii of convergence.

  4. Predict the coefficients of x8x^8 in uu and x9x^9 in vv. Can an additional exact measurement assigning the value 1/201/20 to the former coefficient be consistent with the equation and the original data?

Original worksheet page 1: question and worked solution for 6-3-008
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Question 8 – Solution

Strategy. Infer the differential operator from low-order data, then validate all orders by a transformation.

Step 1: Recover the three constants. The constant coefficient in the equation for uu gives −2+β=0-2+\beta=0. The xx coefficient for vv gives −6+α+β=0-6+\alpha+\beta=0. The x2x^2 coefficient for uu gives 6−2α−β+γ=06-2\alpha-\beta+\gamma=0. These successive equations uniquely force β=2,α=4,γ=4.\boxed{\beta=2,\qquad\alpha=4,\qquad\gamma=4.}

Step 2: State a recurrence valid from the start. With a−2=a−1=0a_{-2}=a_{-1}=0 for the shifted contribution, an+2=−(4n+2)an+4an−2(n+2)(n+1)(n≥0).\boxed{a_{n+2}=-\frac{(4n+2)a_n+4a_{n-2}}{(n+2)(n+1)}\quad(n\ge 0).} The starting coefficients a0=y(0)a_0=y(0) and a1=y′(0)a_1=y'(0) are free. In particular, a2=−a0a_2=-a_0 and a3=−a1a_3=-a_1; no negative-index coefficient is an additional parameter.

Step 3: Verify the recovered equation globally. Writing E=e−x2E=e^{-x^2}, differentiation gives y′=E(w′−2xw),y″=E(w″−4xw′+(4x2−2)w).y'=E(w'-2xw),\qquad y''=E\big(w''-4xw'+(4x^2-2)w\big). Thus y″+4xy′+(2+4x2)y=Ew″y''+4xy'+(2+4x^2)y=Ew''. The equation becomes w″=0w''=0, yielding y=e−x2(C1+C2x),u=e−x2,v=xe−x2.\boxed{y=e^{-x^2}(C_1+C_2x),\quad u=e^{-x^2},\quad v=xe^{-x^2}.} Their initial data match the measured series, and their Wronskian is E2=e−2x2>0E^2=e^{-2x^2}>0. Both functions are entire, so both Taylor radii are infinite. The transformation also proves the entire measured series, not just the first displayed terms, are consistent.

Step 4: Test a new exact measurement. The exponential expansion gives [x8]u=1/4!=1/24[x^8]u=1/4!=1/24 and [x9]v=1/24[x^9]v=1/24. The recurrence produces the same values. Since the recovered parameters and each solution’s initial data are fixed uniquely, 1/201/20 is incompatible; it cannot be accommodated by choosing later coefficients independently.

Original worksheet page 2: question and worked solution for 6-3-008

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