Question #66661

Find the integrating factor of the differential equation
(6xy-3y^2+2y) dx + 2(x-y) dy =0
and hence solve it

Expert's answer

Answer on Question #66661 – Math – Differential Equations

Question

Find the integrating factor of the differential equation


(6xy3y2+2y)dx+2(xy)dy=0(6xy - 3y^2 + 2y) \, dx + 2(x - y) \, dy = 0


and hence solve it.

Solution

P(x,y)dx+Q(x,y)dy=0, whereP(x, y) \, dx + Q(x, y) \, dy = 0, \text{ where}P(x,y)=6xy3y2+2y and Q(x,y)=2(xy)P(x, y) = 6xy - 3y^2 + 2y \text{ and } Q(x, y) = 2(x - y)


First, we need to check whether


Py=Qx.\frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x}.Py=6x6y+22=Qx;\frac{\partial P}{\partial y} = 6x - 6y + 2 \neq 2 = \frac{\partial Q}{\partial x};PyQx=6x6y+22=6x6y=6(xy)\frac{\partial P}{\partial y} - \frac{\partial Q}{\partial x} = 6x - 6y + 2 - 2 = 6x - 6y = 6(x - y)


It can be noticed that


1Q(PyQx)=6(xy)2(xy)=3\frac{1}{Q} \left( \frac{\partial P}{\partial y} - \frac{\partial Q}{\partial x} \right) = \frac{6(x - y)}{2(x - y)} = 3


that means our integrating factor as a function depends on xx only:


μ=μ(x).\mu = \mu(x).


We can find it from the equation:


1μdμdx=1Q(PyQx)=3\frac{1}{ \mu} \frac{d\mu}{dx} = \frac{1}{Q} \left( \frac{\partial P}{\partial y} - \frac{\partial Q}{\partial x} \right) = 3dμμ=3dx\frac{d\mu}{\mu} = 3 \, dxdμμ=3dx\int \frac{d\mu}{\mu} = 3 \int dxlnμ=3x+lnC\ln |\mu| = 3x + \ln |C|μ=Ce3x,\mu = C e^{3x},


but we will take the integrating factor


μ=e3x\mu = e^{3x}


Now, we have


e3x(6xy3y2+2y)dx+2e3x(xy)dy=0\mathrm{e}^{3x}(6xy - 3y^2 + 2y)\mathrm{dx} + 2\mathrm{e}^{3x}(x - y)\mathrm{dy} = 0P(x,y)=e3x(6xy3y2+2y) and Q(x,y)=2e3x(xy)P(x, y) = \mathrm{e}^{3x}(6xy - 3y^2 + 2y) \text{ and } Q(x, y) = 2\mathrm{e}^{3x}(x - y)Py=e3x(6x6y+2)=e3x(6y+2+6x)=Qx\frac{\partial P}{\partial y} = \mathrm{e}^{3x}(6x - 6y + 2) = \mathrm{e}^{3x}(-6y + 2 + 6x) = \frac{\partial Q}{\partial x}


So, u(x,y):{ux=e3x(6xy3y2+2y)uy=2e3x(xy)\exists u(x,y): \begin{cases} \dfrac{\partial u}{\partial x} = \mathrm{e}^{3x}(6xy - 3y^2 + 2y) \\ \dfrac{\partial u}{\partial y} = 2\mathrm{e}^{3x}(x - y) \end{cases}

u(x,y)=e3x(6xy3y2+2y)dx+φ(y)=136xyd(e3x)+13e3x(3y2+2y)+φ(y)==e3x2xy13e3xd(6xy)+13e3x(3y2+2y)+φ(y)==e3x2xy2e3xydx+13e3x(3y2+2y)+φ(y)==e3x(2xy23yy2+23y)+φ(y)=e3x(2xyy2)+φ(y)\begin{aligned} u(x, y) &= \int \mathrm{e}^{3x}(6xy - 3y^2 + 2y)\mathrm{dx} + \varphi(y) \\ &= \frac{1}{3} \int 6xyd(\mathrm{e}^{3x}) + \frac{1}{3}\mathrm{e}^{3x}(-3y^2 + 2y) + \varphi(y) = \\ &= \mathrm{e}^{3x}2xy - \frac{1}{3} \int \mathrm{e}^{3x}d(6xy) + \frac{1}{3}\mathrm{e}^{3x}(-3y^2 + 2y) + \varphi(y) = \\ &= \mathrm{e}^{3x}2xy - 2 \int \mathrm{e}^{3x}y\mathrm{dx} + \frac{1}{3}\mathrm{e}^{3x}(-3y^2 + 2y) + \varphi(y) = \\ &= \mathrm{e}^{3x}\left(2xy - \frac{2}{3}y - y^2 + \frac{2}{3}y\right) + \varphi(y) = \mathrm{e}^{3x}(2xy - y^2) + \varphi(y) \\ \end{aligned}uy=y(e3x(2xyy2)+φ(y))=2e3x(xy)e3x(2x2y)+φ(y)=2e3x(xy)φ(y)=0φ(y)=Cu(x,y)=e3x(2xyy2)+C=0,\begin{aligned} \frac{\partial u}{\partial y} &= \frac{\partial}{\partial y}\left(\mathrm{e}^{3x}(2xy - y^2) + \varphi(y)\right) = 2\mathrm{e}^{3x}(x - y) \\ \mathrm{e}^{3x}(2x - 2y) + \varphi'(y) &= 2\mathrm{e}^{3x}(x - y) \\ \varphi'(y) &= 0 \\ \varphi(y) &= C \\ u(x, y) &= \mathrm{e}^{3x}(2xy - y^2) + C = 0, \end{aligned}


where CC is an arbitrary real constant.

Answer: u(x,y)=e3x(2xyy2)+C=0u(x, y) = \mathrm{e}^{3x}(2xy - y^2) + C = 0.

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