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Separable differential equations, which are also first order, are of the form

\displaystyle \cfrac{dy}{dx} =f(x)g(y)

The method to solve separable differential equations is to put variables of x on one side of the equation and variables of y on the other side of the equal sign.

\displaystyle \cfrac{dy}{g(y)} =f(x)dx

Integrate each side as an indefinite integral and remember to include the combined integration constant.

\displaystyle \int \cfrac{dy}{g(y)} =\int f(x)dx

A final step is to solve for y as a function of x if possible, otherwise just leave the result as an implicit relationship.

Or to avoid using integration constants requires knowing

\displaystyle x_{1} ,x_{2},y_{1},y_{2}

In this case,

\displaystyle \int_{y_{1} }^{y_{2} }\cfrac{dy}{g(y)}=\int_{x_{1} }^{x_{2} }f(x)dx

is the solution.


Example 1. Solve the following differential equation

\displaystyle \cfrac{dy}{dx} =\sin x\sqrt{1-y^{2} }

Solution 1. We first separate the variables.

\displaystyle \cfrac{dy}{\sqrt{1-y^{2} } } =\sin xdx

Then we take the indefinite integral

\displaystyle \int \cfrac{dy}{\sqrt{1-y^2}}=\int \sin xdx

The result is

\displaystyle \arcsin y=-\cos x+C

It is usual to solve for y if possible. In this case, we write

\displaystyle y=\sin (C-\cos x)


Example 2. Solve the following differential equation

\displaystyle \cfrac{dy}{dx} =xe^{x-y}

Solution 2. First separate the variables,

\displaystyle e^y dy =xe^x dx

then take the indefinite integral of both sides

\displaystyle \int e^y dy=\int xe^x dx
\displaystyle e^y =xe^x -e^x + C

In the last step, solve for y

\displaystyle y = \ln (xe^x - e^x + C)

If there is an initial value problem for this differential equation we could determine the integration constant. Let us define a typical initial value problem as y(0)=1. This gives an equation for the constant in the previous solution

\displaystyle 1=\ln (C-1)
 C = e + 1


Example 3. Another type of equation which technically is separable is when

\displaystyle \cfrac{dy}{dx}=0

Solution 3. We can integrate both the left and right hand sides of the equation with respect to $x$ and we get.

\displaystyle \int\cfrac{dy}{dx}=\int 0dx\qquad y=C

Another possible generalization of the previous equation is

\displaystyle \cfrac{d^{3} y}{dx^3}=0
\displaystyle \cfrac{d^{2} y}{dx^{2} }=a
\displaystyle \cfrac{dy}{dx}=ax+b
\displaystyle y = \cfrac{a}{2} x^{2}+bx+c

Other possible separable equations when g(y)=1 might look like

\displaystyle \cfrac{d^{n} y}{dx^{n} } =f(x)

Here, we just integrate both sides, n times with respect to x. After each integration, a new integration constant appears in the antiderivative.

Here we have used integration constants corresponding to the physics problem of vertical projectile motion.

\displaystyle \cfrac{d^{2} y}{dt^{2} }=-g
\displaystyle \cfrac{dy}{dt}=-gt+v_{0}
\displaystyle y = y_0 + v_0 t-\cfrac{1}{2} gt^2

Or try this differential equation

\displaystyle \cfrac{d^{2}y}{dx^2 } = \cos x
\cfrac{dy}{dx}= \sin x+A
y=-\cos x+Ax+B

Separable equations are some of the most straightforward differential equations to solve because all that is required is normal integration.

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Previous Topic: Introduction to Differential Equations

Next Topic: First Order Linear Differential Equations


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