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Solve the nonlinear differential equation yy'' + (y')² = ky'

Mathematics

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Answer

yk−C1k2ln⁡∣ky+C1∣=x+C2\frac{y}{k} - \frac{C_1}{k^2} \ln|ky + C_1| = x + C_2

y=Cy = C

y2=Ax+By^2 = Ax + B

Step-by-step solution

3 steps

To solve the nonlinear differential equation yy′′+(y′)2=ky′yy'' + (y')^2 = ky':

  1. Rewrite the equation.

    The given differential equation is yy′′+(y′)2=ky′yy'' + (y')^2 = ky'.
    Notice that the left side of the equation is the derivative of the product yy′yy' with respect to xx:

    ddx(yy′)=y′′y+y′y′=yy′′+(y′)2\frac{d}{dx}(yy') = y''y + y'y' = yy'' + (y')^2

    So, the differential equation can be rewritten as:

    ddx(yy′)=ky′\frac{d}{dx}(yy') = ky'
  2. Integrate with respect to xx.

    Integrate both sides of the equation with respect to xx:

    ∫ddx(yy′)dx=∫ky′dx\int \frac{d}{dx}(yy') dx = \int ky' dx yy′=k∫y′dxyy' = k \int y' dx yy′=ky+C1yy' = ky + C_1

    where C1C_1 is an arbitrary constant of integration.

  3. Solve the first-order separable differential equation yy′=ky+C1y y' = ky + C_1.

    Case 1: k≠0k \neq 0.
    The equation is ydydx=ky+C1y \frac{dy}{dx} = ky + C_1.
    Separate the variables:

    yky+C1dy=dx\frac{y}{ky + C_1} dy = dx

    Integrate both sides:

    ∫yky+C1dy=∫dx\int \frac{y}{ky + C_1} dy = \int dx

    To integrate the left side, we use algebraic manipulation:

    ∫1k(1−C1ky+C1)dy=x+C2\int \frac{1}{k} \left(1 - \frac{C_1}{ky + C_1}\right) dy = x + C_2 1k(y−C1∫1ky+C1dy)=x+C2\frac{1}{k} \left(y - C_1 \int \frac{1}{ky + C_1} dy\right) = x + C_2 1k(y−C1kln⁡∣ky+C1∣)=x+C2\frac{1}{k} \left(y - \frac{C_1}{k} \ln|ky + C_1|\right) = x + C_2 yk−C1k2ln⁡∣ky+C1∣=x+C2\frac{y}{k} - \frac{C_1}{k^2} \ln|ky + C_1| = x + C_2

    This is the general implicit solution for k≠0k \neq 0.
    Additionally, if ky+C1=0ky + C_1 = 0, then y=−C1ky = -\frac{C_1}{k}, which is a constant solution. Let C=−C1kC = -\frac{C_1}{k}. Then y=Cy=C is a solution. Substituting y=Cy=C into the original differential equation gives C(0)+(0)2=k(0)C(0) + (0)^2 = k(0), which is 0=00=0. This constant solution y=Cy=C is a singular solution not covered by the implicit form due to the logarithm.

    Case 2: k=0k = 0.
    If k=0k=0, the equation from Step 2 becomes yy′=C1yy' = C_1.

    ydydx=C1y \frac{dy}{dx} = C_1

    Separate the variables:

    ydy=C1dxy dy = C_1 dx

    Integrate both sides:

    ∫ydy=∫C1dx\int y dy = \int C_1 dx 12y2=C1x+C2\frac{1}{2} y^2 = C_1 x + C_2 y2=2C1x+2C2y^2 = 2C_1 x + 2C_2

    Let A=2C1A = 2C_1 and B=2C2B = 2C_2.

    y2=Ax+By^2 = Ax + B

    This is the general implicit solution for k=0k=0. The constant solution y=Cy=C is covered by this form when A=0A=0, giving y2=By^2=B, so y=±By=\pm\sqrt{B}.

    The solutions are:
    For k≠0k \neq 0:

    yk−C1k2ln⁡∣ky+C1∣=x+C2\boxed{\frac{y}{k} - \frac{C_1}{k^2} \ln|ky + C_1| = x + C_2}

    And the singular solution:

    y=C\boxed{y = C}

    For k=0k = 0:

    y2=Ax+B\boxed{y^2 = Ax + B}
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