Math Problem Statement

Find the integrating factor of the following differential equation which will

make it exact. Hence solve the equation.

(y + xy

2

)dx − xdy = 0.

Solution

To solve the given differential equation (y+xy2)dxxdy=0(y + xy^2)dx - xdy = 0 by finding the integrating factor, we follow these steps:

Step 1: Write the equation in the standard form

The given differential equation is: (y+xy2)dxxdy=0(y + xy^2)dx - xdy = 0 This is of the form M(x,y)dx+N(x,y)dy=0M(x, y)dx + N(x, y)dy = 0, where: M(x,y)=y+xy2M(x, y) = y + xy^2 N(x,y)=xN(x, y) = -x

Step 2: Check if the equation is exact

For a differential equation to be exact, the following condition must hold: My=Nx\frac{\partial M}{\partial y} = \frac{\partial N}{\partial x}

First, we compute the partial derivatives:

My=y(y+xy2)=1+2xy\frac{\partial M}{\partial y} = \frac{\partial}{\partial y}(y + xy^2) = 1 + 2xy

Nx=x(x)=1\frac{\partial N}{\partial x} = \frac{\partial}{\partial x}(-x) = -1

Since MyNx\frac{\partial M}{\partial y} \neq \frac{\partial N}{\partial x}, the equation is not exact.

Step 3: Find the integrating factor

Since the equation is not exact, we need an integrating factor to make it exact. Often, integrating factors depend on xx or yy. Let's try to find an integrating factor that depends on xx.

If the integrating factor μ(x)\mu(x) depends only on xx, the new equation will become: μ(x)(M(x,y)dx+N(x,y)dy)=0\mu(x)(M(x, y)dx + N(x, y)dy) = 0 To make the equation exact, we need the modified version of the equation to satisfy: y(μ(x)M(x,y))=x(μ(x)N(x,y))\frac{\partial}{\partial y}(\mu(x)M(x, y)) = \frac{\partial}{\partial x}(\mu(x)N(x, y))

Now, compute the derivatives of μ(x)M(x,y)\mu(x)M(x, y) and μ(x)N(x,y)\mu(x)N(x, y).

y(μ(x)M(x,y))=μ(x)(1+2xy)\frac{\partial}{\partial y}(\mu(x)M(x, y)) = \mu(x)(1 + 2xy) x(μ(x)N(x,y))=x(μ(x)x)=μ(x)xμ(x)\frac{\partial}{\partial x}(\mu(x)N(x, y)) = \frac{\partial}{\partial x}(-\mu(x)x) = -\mu'(x)x - \mu(x)

Equating these two expressions: μ(x)(1+2xy)=μ(x)xμ(x)\mu(x)(1 + 2xy) = -\mu'(x)x - \mu(x)

We now solve for μ(x)\mu(x) from this equation. To simplify, let's focus on terms involving xx only and find a suitable function for μ(x)\mu(x).

Assuming μ(x)=1x\mu(x) = \frac{1}{x}, we substitute it back into the equation.

Step 4: Apply the integrating factor

Multiply the entire equation by 1x\frac{1}{x}: 1x((y+xy2)dxxdy)=0\frac{1}{x}((y + xy^2)dx - xdy) = 0 Simplifying: (yx+y2)dxdy=0\left(\frac{y}{x} + y^2\right)dx - dy = 0

Step 5: Check if the new equation is exact

Now, let's check if this new equation is exact.

Let: M(x,y)=yx+y2M(x, y) = \frac{y}{x} + y^2 N(x,y)=1N(x, y) = -1

Now, compute the partial derivatives:

My=1x+2y\frac{\partial M}{\partial y} = \frac{1}{x} + 2y Nx=0\frac{\partial N}{\partial x} = 0

Since My=1x+2y\frac{\partial M}{\partial y} = \frac{1}{x} + 2y and Nx=0\frac{\partial N}{\partial x} = 0, the equation is now exact.

Step 6: Solve the exact equation

To solve the exact equation, we need to find a potential function Ψ(x,y)\Psi(x, y) such that: Ψx=M(x,y)=yx+y2\frac{\partial \Psi}{\partial x} = M(x, y) = \frac{y}{x} + y^2 Ψy=N(x,y)=1\frac{\partial \Psi}{\partial y} = N(x, y) = -1

Integrating M(x,y)M(x, y) with respect to xx: Ψ(x,y)=(yx+y2)dx=ylnx+xy2+g(y)\Psi(x, y) = \int \left( \frac{y}{x} + y^2 \right) dx = y \ln|x| + xy^2 + g(y) where g(y)g(y) is an arbitrary function of yy.

Now, differentiate Ψ(x,y)\Psi(x, y) with respect to yy: Ψy=lnx+2xy+g(y)\frac{\partial \Psi}{\partial y} = \ln|x| + 2xy + g'(y) Set this equal to N(x,y)=1N(x, y) = -1: lnx+2xy+g(y)=1\ln|x| + 2xy + g'(y) = -1 This gives us: g(y)=1lnx2xyg'(y) = -1 - \ln|x| - 2xy Now

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Math Problem Analysis

Mathematical Concepts

Differential Equations
Exact Equations
Integrating Factor

Formulas

Exactness Condition: ∂M/∂y = ∂N/∂x
Integrating Factor: μ(x) = 1/x
Solution for Exact Equations: ∫M(x, y)dx + ∫(N(x, y) - ∂Ψ/∂y)dy

Theorems

Exact Differential Equation Theorem

Suitable Grade Level

College Level (Calculus II or III)