Solve: dy/dx+ y = xy^3 .??

Answer 1

#y = pm 1/sqrt( x + 1/2 + C e^(2x))#

#dy/dx+ y = xy^3#

This is non-linear but we can make it linear using a Bernoulli substitution. Here we let:

Multiply both sides of the DE by #- 2/y^3#:
#underbrace(dy/dx * (- 2/y^3))_(= z')+ underbrace(y* (- 2/y^3))_(= - 2z) = underbrace(xy^3 * (- 2/y^3))_(= - 2x) #
For this, the integrating factor is: #exp(int (-2) dx) = e^(-2x)#
#e^(- 2x) (z' - 2z) [=(e^(- 2x) z)^'] = - 2xe^(- 2x)#

Integrating both sides, using IBP on RHS:

#e^(- 2x) z = int \ x \ d( e^(- 2x))#
#e^(- 2x) z = \ x \ e^(- 2x) - int dx \ e^(- 2x)#
#e^(- 2x) z = x e^(- 2x) + 1/2 \ e^(- 2x) + C#
# z = x + 1/2 + C e^(2x) qquad = 1/y^2#
#y = pm 1/sqrt( x + 1/2 + C e^(2x))#
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Answer 2

This is a first-order nonlinear ordinary differential equation. To solve it, we can use the method of separation of variables.

  1. Rewrite the equation in the form ( \frac{dy}{dx} = xy^3 - y ).
  2. Factor out (y) on the right side to get ( \frac{dy}{dx} = y(x y^2 - 1) ).
  3. Now, separate variables: ( \frac{1}{y} dy = (x y^2 - 1) dx ).
  4. Integrate both sides. The integral of ( \frac{1}{y} dy ) is ( \ln|y| ), and the integral of ( (x y^2 - 1) dx ) requires a substitution.
  5. Solve the resulting integrals to find the general solution.

This process will lead to the solution of the given differential equation.

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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