Bernoulli Differential Equations — Question 4

Section 21-4 · Calculus pages 3727–3728

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Question 4

Consider the negative-power Bernoulli equation y′+y=e−xy,y(0)=−1.y'+y=\frac{e^{-x}}y,\qquad y(0)=-1. The original equation is defined only when y≠0y\ne 0.

Tasks

  1. Derive the linear equation for v=y2v=y^2 and solve it using the initial condition.

  2. Select the real branch for yy and find its maximal interval containing 00.

  3. Determine what happens to yy and y′y' at its finite endpoint. Decide whether reaching the value zero permits continuation.

  4. Verify the equation, and explain why the zero function cannot be restored as an omitted solution in this example.

Question 4 – Solution

Strategy. The squared variable must be strictly positive, and the original reciprocal term remains undefined at zero.

Step 1: Linearize and integrate. Multiplication by 2y2y yields v′+2v=2e−xv'+2v=2e^{-x}, where v=y2v=y^2. Using the integrating factor e2xe^{2x}, (e2xv)′=2ex,v=2e−x+Ce−2x.(e^{2x}v)'=2e^x,\qquad v=2e^{-x}+Ce^{-2x}. Since v(0)=1v(0)=1, C=−1C=-1.

Step 2: Invert on the correct interval. The condition v=e−2x(2ex−1)>0v=e^{-2x}(2e^x-1)>0 requires x>−ln⁡2x>-\ln 2. The initial sign gives y=−e−x2ex−1,I=(−ln⁡2,∞).\boxed{y=-e^{-x}\sqrt{2e^x-1},\qquad I=(-\ln 2,\infty)}. As x↓−ln⁡2x\downarrow-\ln 2, y→0y\to 0 from below. The equation gives y′=e−x/y−y→−∞y'=e^{-x}/y-y\to-\infty, so no differentiable extension exists at that endpoint. Also the original right-hand side is undefined there. As x→∞x\to\infty, y→0y\to 0 from below, but it never reaches zero at a finite point of II.

Step 3: Verify and check the excluded value. Differentiating y2=vy^2=v gives 2yy′=v′2yy'=v'. Since v′+2v=2e−xv'+2v=2e^{-x} and y≠0y\ne 0 on II, division by 2y2y recovers y′+y=e−x/yy'+y=e^{-x}/y. The selected formula gives y(0)=−1y(0)=-1. Unlike positive-power examples, y≡0 is not a solution\boxed{y\equiv 0\text{ is not a solution}}: the original equation has no value at zero.

Diagram shown in the original SVG worksheet.