Answer on Question #66661 – Math – Differential Equations
Question
Find the integrating factor of the differential equation
( 6 x y − 3 y 2 + 2 y ) d x + 2 ( x − y ) d y = 0 (6xy - 3y^2 + 2y) \, dx + 2(x - y) \, dy = 0 ( 6 x y − 3 y 2 + 2 y ) d x + 2 ( x − y ) d y = 0
and hence solve it.
Solution
P ( x , y ) d x + Q ( x , y ) d y = 0 , where P(x, y) \, dx + Q(x, y) \, dy = 0, \text{ where} P ( x , y ) d x + Q ( x , y ) d y = 0 , where P ( x , y ) = 6 x y − 3 y 2 + 2 y and Q ( x , y ) = 2 ( x − y ) P(x, y) = 6xy - 3y^2 + 2y \text{ and } Q(x, y) = 2(x - y) P ( x , y ) = 6 x y − 3 y 2 + 2 y and Q ( x , y ) = 2 ( x − y )
First, we need to check whether
∂ P ∂ y = ∂ Q ∂ x . \frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x}. ∂ y ∂ P = ∂ x ∂ Q . ∂ P ∂ y = 6 x − 6 y + 2 ≠ 2 = ∂ Q ∂ x ; \frac{\partial P}{\partial y} = 6x - 6y + 2 \neq 2 = \frac{\partial Q}{\partial x}; ∂ y ∂ P = 6 x − 6 y + 2 = 2 = ∂ x ∂ Q ; ∂ P ∂ y − ∂ Q ∂ x = 6 x − 6 y + 2 − 2 = 6 x − 6 y = 6 ( x − y ) \frac{\partial P}{\partial y} - \frac{\partial Q}{\partial x} = 6x - 6y + 2 - 2 = 6x - 6y = 6(x - y) ∂ y ∂ P − ∂ x ∂ Q = 6 x − 6 y + 2 − 2 = 6 x − 6 y = 6 ( x − y )
It can be noticed that
1 Q ( ∂ P ∂ y − ∂ Q ∂ x ) = 6 ( x − y ) 2 ( x − y ) = 3 \frac{1}{Q} \left( \frac{\partial P}{\partial y} - \frac{\partial Q}{\partial x} \right) = \frac{6(x - y)}{2(x - y)} = 3 Q 1 ( ∂ y ∂ P − ∂ x ∂ Q ) = 2 ( x − y ) 6 ( x − y ) = 3
that means our integrating factor as a function depends on x x x only:
μ = μ ( x ) . \mu = \mu(x). μ = μ ( x ) .
We can find it from the equation:
1 μ d μ d x = 1 Q ( ∂ P ∂ y − ∂ Q ∂ x ) = 3 \frac{1}{ \mu} \frac{d\mu}{dx} = \frac{1}{Q} \left( \frac{\partial P}{\partial y} - \frac{\partial Q}{\partial x} \right) = 3 μ 1 d x d μ = Q 1 ( ∂ y ∂ P − ∂ x ∂ Q ) = 3 d μ μ = 3 d x \frac{d\mu}{\mu} = 3 \, dx μ d μ = 3 d x ∫ d μ μ = 3 ∫ d x \int \frac{d\mu}{\mu} = 3 \int dx ∫ μ d μ = 3 ∫ d x ln ∣ μ ∣ = 3 x + ln ∣ C ∣ \ln |\mu| = 3x + \ln |C| ln ∣ μ ∣ = 3 x + ln ∣ C ∣ μ = C e 3 x , \mu = C e^{3x}, μ = C e 3 x ,
but we will take the integrating factor
μ = e 3 x \mu = e^{3x} μ = e 3 x
Now, we have
e 3 x ( 6 x y − 3 y 2 + 2 y ) d x + 2 e 3 x ( x − y ) d y = 0 \mathrm{e}^{3x}(6xy - 3y^2 + 2y)\mathrm{dx} + 2\mathrm{e}^{3x}(x - y)\mathrm{dy} = 0 e 3 x ( 6 x y − 3 y 2 + 2 y ) dx + 2 e 3 x ( x − y ) dy = 0 P ( x , y ) = e 3 x ( 6 x y − 3 y 2 + 2 y ) and Q ( x , y ) = 2 e 3 x ( x − y ) P(x, y) = \mathrm{e}^{3x}(6xy - 3y^2 + 2y) \text{ and } Q(x, y) = 2\mathrm{e}^{3x}(x - y) P ( x , y ) = e 3 x ( 6 x y − 3 y 2 + 2 y ) and Q ( x , y ) = 2 e 3 x ( x − y ) ∂ P ∂ y = e 3 x ( 6 x − 6 y + 2 ) = e 3 x ( − 6 y + 2 + 6 x ) = ∂ Q ∂ x \frac{\partial P}{\partial y} = \mathrm{e}^{3x}(6x - 6y + 2) = \mathrm{e}^{3x}(-6y + 2 + 6x) = \frac{\partial Q}{\partial x} ∂ y ∂ P = e 3 x ( 6 x − 6 y + 2 ) = e 3 x ( − 6 y + 2 + 6 x ) = ∂ x ∂ Q
So, ∃ u ( x , y ) : { ∂ u ∂ x = e 3 x ( 6 x y − 3 y 2 + 2 y ) ∂ u ∂ y = 2 e 3 x ( x − y ) \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 ) : ⎩ ⎨ ⎧ ∂ x ∂ u = e 3 x ( 6 x y − 3 y 2 + 2 y ) ∂ y ∂ u = 2 e 3 x ( x − y )
u ( x , y ) = ∫ e 3 x ( 6 x y − 3 y 2 + 2 y ) d x + φ ( y ) = 1 3 ∫ 6 x y d ( e 3 x ) + 1 3 e 3 x ( − 3 y 2 + 2 y ) + φ ( y ) = = e 3 x 2 x y − 1 3 ∫ e 3 x d ( 6 x y ) + 1 3 e 3 x ( − 3 y 2 + 2 y ) + φ ( y ) = = e 3 x 2 x y − 2 ∫ e 3 x y d x + 1 3 e 3 x ( − 3 y 2 + 2 y ) + φ ( y ) = = e 3 x ( 2 x y − 2 3 y − y 2 + 2 3 y ) + φ ( y ) = e 3 x ( 2 x y − y 2 ) + 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} u ( x , y ) = ∫ e 3 x ( 6 x y − 3 y 2 + 2 y ) dx + φ ( y ) = 3 1 ∫ 6 x y d ( e 3 x ) + 3 1 e 3 x ( − 3 y 2 + 2 y ) + φ ( y ) = = e 3 x 2 x y − 3 1 ∫ e 3 x d ( 6 x y ) + 3 1 e 3 x ( − 3 y 2 + 2 y ) + φ ( y ) = = e 3 x 2 x y − 2 ∫ e 3 x y dx + 3 1 e 3 x ( − 3 y 2 + 2 y ) + φ ( y ) = = e 3 x ( 2 x y − 3 2 y − y 2 + 3 2 y ) + φ ( y ) = e 3 x ( 2 x y − y 2 ) + φ ( y ) ∂ u ∂ y = ∂ ∂ y ( e 3 x ( 2 x y − y 2 ) + φ ( y ) ) = 2 e 3 x ( x − y ) e 3 x ( 2 x − 2 y ) + φ ′ ( y ) = 2 e 3 x ( x − y ) φ ′ ( y ) = 0 φ ( y ) = C u ( x , y ) = e 3 x ( 2 x y − y 2 ) + 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} ∂ y ∂ u e 3 x ( 2 x − 2 y ) + φ ′ ( y ) φ ′ ( y ) φ ( y ) u ( x , y ) = ∂ y ∂ ( e 3 x ( 2 x y − y 2 ) + φ ( y ) ) = 2 e 3 x ( x − y ) = 2 e 3 x ( x − y ) = 0 = C = e 3 x ( 2 x y − y 2 ) + C = 0 ,
where C C C is an arbitrary real constant.
Answer: u ( x , y ) = e 3 x ( 2 x y − y 2 ) + C = 0 u(x, y) = \mathrm{e}^{3x}(2xy - y^2) + C = 0 u ( x , y ) = e 3 x ( 2 x y − y 2 ) + C = 0 .
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