Final Thoughts — Question 6

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Question 6

Compare an equation with its squared version: (A)y′=−1−y2,|y|≤1,\text{(A)}\quad y'=-\sqrt{1-y^2},\qquad |y|\le 1, (B)(y′)2=1−y2.\text{(B)}\quad (y')^2=1-y^2. Both are assigned y(0)=0y(0)=0. Consider u(x)=sin⁡xu(x)=\sin x and v(x)=−sin⁡xv(x)=-\sin x.

Tasks

  1. Verify that both candidates satisfy (B) and the initial value. Which satisfies (A) on (−π/2,π/2)(-\pi/2,\pi/2)?

  2. State the sign restriction lost by squaring. Give a condition that, together with (B), recovers (A) for real differentiable functions.

  3. Explain why v=−sin⁡xv=-\sin x does not satisfy (A) on all of ℝ\mathbb R.

  4. Extend the accepted middle branch to a C1C^1 solution of (A) on all of ℝ\mathbb R by adjoining constant pieces outside [−π/2,π/2][-\pi/2,\pi/2]. Verify the joins and sketch the extension in your solution.

Original worksheet page 1: question and worked solution for 1-3-006
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Question 6 – Solution

Strategy. Squaring forgets a sign. Restore that sign when selecting a branch, and check differentiability when extending it.

Step 1: Compare the candidates. Both satisfy (y′)2=cos⁡2x=1−y2(y')^2=\cos^2x=1-y^2 and have value zero at 00. On (−π/2,π/2)(-\pi/2,\pi/2), cos⁡x>0\cos x>0, so the right-hand side of (A) is −|cos⁡x|=−cos⁡x-|\cos x|=-\cos x. Hence v=−sin⁡x satisfies (A), but u=sin⁡x does not.\boxed{v=-\sin x\text{ satisfies (A), but }u=\sin x\text{ does not.}}

Step 2: Recover the lost information. Equation (A) forces y′≤0y'\le 0. Conversely, (B) and y′≤0y'\le 0 imply |y|≤1|y|\le 1 and y′=−1−y2y'=-\sqrt{1-y^2}. Outside the middle interval, v′=−cos⁡xv'=-\cos x is positive wherever cos⁡x<0\cos x<0, so vv fails (A) there.

Step 3: A global extension. Define Y(x)={1,x≤−π/2,−sin⁡x,−π/2<x<π/2,−1,x≥π/2.\boxed{Y(x)=\begin{cases} 1,&x\le-\pi/2,\\ -\sin x,&-\pi/2<x<\pi/2,\\ -1,&x\ge\pi/2. \end{cases}}

See the diagram in the original worksheet below.

At either join, the middle value matches the adjoining constant and its derivative −cos⁡x-\cos x tends to zero, the derivative of the constant piece. Thus YY is C1C^1. On the constant pieces and at the joins, both sides of (A) are zero. On the middle piece, the verification above applies. Therefore YY solves the original IVP on ℝ\mathbb R; extension is possible here because both endpoint values and derivatives remain finite.

Original worksheet page 2: question and worked solution for 1-3-006

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