Variation of Parameters — Question 2

Section 22-10 · Calculus pages 4023–4024

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Question 2

Solve on I=(−π/2,π/2)I=(-\pi/2,\pi/2): y″+y=sec⁡t,y(0)=y′(0)=0.y''+y=\sec t,\qquad y(0)=y'(0)=0. Use the homogeneous pair cos⁡t,sin⁡t\cos t,\sin t.

Tasks

  1. Derive the parameter derivatives and evaluate the integrals with lower endpoint zero.

  2. Simplify the initial-value solution and verify its equation and both data.

  3. Determine the limits of yy and y′y' as t→(π/2)−t\to(\pi/2)^-. Can the solution extend as a C1C^1 function through that endpoint?

  4. Explain why a finite limit of yy does not enlarge the interval on which this initial-value problem has a classical solution.

Question 2 – Solution

Strategy. The forcing is singular at the interval endpoints. Keep its domain visible even when the solution itself has a finite limit.

Step 1: Integrate the parameter system. Here W=1W=1. The equations u1′cos⁡t+u2′sin⁡t=0u_1'\cos t+u_2'\sin t=0 and −u1′sin⁡t+u2′cos⁡t=sec⁡t-u_1'\sin t+u_2'\cos t=\sec t give u1′=−tan⁡t,u2′=1.u_1'=-\tan t,\qquad u_2'=1. Since cos⁡t>0\cos t>0 on II, integration from zero yields u1=ln⁡(cos⁡t)u_1=\ln(\cos t), u2=tu_2=t.

Step 2: Verify the response. The zero lower endpoints fit both data, and y=cos⁡tln⁡(cos⁡t)+tsin⁡t.\boxed{y=\cos t\ln(\cos t)+t\sin t.} Differentiation simplifies to y′=−sin⁡tln⁡(cos⁡t)+tcos⁡t,y″=−cos⁡tln⁡(cos⁡t)+sin⁡2tcos⁡t+cos⁡t−tsin⁡t.y'=-\sin t\ln(\cos t)+t\cos t, \quad y''=-\cos t\ln(\cos t)+\frac{\sin^2t}{\cos t}+\cos t-t\sin t. Therefore y″+y=(sin⁡2t+cos⁡2t)/cos⁡t=sec⁡ty''+y=(\sin^2t+\cos^2t)/\cos t=\sec t, and both data vanish.

Step 3: Examine the endpoint. Using xln⁡x→0x\ln x\to 0 as x→0+x\to 0^+, we obtain limt→(π/2)−y(t)=π/2,limt→(π/2)−y′(t)=+∞.\lim_{t\to(\pi/2)^-}y(t)=\pi/2,\qquad \lim_{t\to(\pi/2)^-}y'(t)=+\infty. Thus even a C1C^1 extension is impossible. The graph approaches a finite height with an unbounded positive slope; the endpoint is excluded.

Step 4: Keep the equation’s domain. The right side sec⁡t\sec t is undefined at π/2\pi/2 and −π/2-\pi/2. A continuous assignment to yy at an endpoint would not define the differential equation there. The maximal open interval containing zero on which this IVP is classical is exactly II.

Diagram shown in the original SVG worksheet.