ANSWER on Question #77405 – Math – Differential Equations
QUESTION
Solve the partial differential equation
( D 2 + 3 D D ′ + 2 D ′ 2 ) z = 12 x y (D^2 + 3DD' + 2D'^2)z = 12xy ( D 2 + 3 D D ′ + 2 D ′2 ) z = 12 x y SOLUTION
Let us use some known facts.
Let the given differential equation be
F ( D , D ′ ) = f ( x , y ) . F(D, D') = f(x, y). F ( D , D ′ ) = f ( x , y ) .
Factorize F ( D , D ′ ) F(D, D') F ( D , D ′ ) into linear factors. Then use the following results:
**Rule I.** Corresponding to each non-repeated factor ( b D − a D ′ − c ) (bD - aD' - c) ( b D − a D ′ − c ) , the part of C.F. is taken as
e ( c x b ) φ ( b y + a x ) , if b ≠ 0 e^{\left(\frac{cx}{b}\right)} \varphi(by + ax), \quad \text{if } b \neq 0 e ( b c x ) φ ( b y + a x ) , if b = 0
We now have three particular cases of Rule I:
**Rule IA.** Take c = 0 c = 0 c = 0 in Rule I. Hence corresponding to each linear factor ( b D − a D ′ ) (bD - aD') ( b D − a D ′ ) , the part of C.F. is
φ ( b y + a x ) , if b ≠ 0. \varphi(by + ax), \quad \text{if } b \neq 0. φ ( b y + a x ) , if b = 0.
**Rule IB.** Take a = 0 a = 0 a = 0 in Rule I. Hence corresponding to each linear factor ( b D − c ) (bD - c) ( b D − c ) , the part of C.F. is
e ( c x b ) φ ( b y ) , if b ≠ 0. e^{\left(\frac{cx}{b}\right)} \varphi(by), \quad \text{if } b \neq 0. e ( b c x ) φ ( b y ) , if b = 0.
**Rule IC.** Take a = c = 0 a = c = 0 a = c = 0 and b = 1 b = 1 b = 1 in Rule I. Hence corresponding to each linear factor ( 1 ⋅ D ) (1 \cdot D) ( 1 ⋅ D ) , the part of C.F. is
φ ( y ) . \varphi(y). φ ( y ) .
In our case,
( D 2 + 3 D D ′ + 2 D ′ 2 ) z = 12 x y → z ( x , y ) = C . F . + P . I . (D^{2} + 3DD' + 2D'^{2})z = 12xy \rightarrow z(x,y) = C.F. + P.I. ( D 2 + 3 D D ′ + 2 D ′ 2 ) z = 12 x y → z ( x , y ) = C . F . + P . I .
0 STEP: We factor the expression
D 2 + 3 D D ′ + 2 D ′ 2 = ( D 2 + D D ′ ) + ( 2 D D ′ + 2 D ′ 2 ) = = D ( D + D ′ ) + 2 D ′ ( D + D ′ ) = ( D + D ′ ) ( D + 2 D ′ ) \begin{aligned}
D^{2} + 3DD' + 2D'^{2} &= (D^{2} + DD') + (2DD' + 2D'^{2}) = \\
&= D(D + D') + 2D'(D + D') = (D + D')(D + 2D')
\end{aligned} D 2 + 3 D D ′ + 2 D ′ 2 = ( D 2 + D D ′ ) + ( 2 D D ′ + 2 D ′ 2 ) = = D ( D + D ′ ) + 2 D ′ ( D + D ′ ) = ( D + D ′ ) ( D + 2 D ′ )
Conclusion,
( D 2 + 3 D D ′ + 2 D ′ 2 ) z = ( D + D ′ ) ( D + 2 D ′ ) z \boxed{(D^{2} + 3DD' + 2D'^{2})z = (D + D')(D + 2D')z} ( D 2 + 3 D D ′ + 2 D ′ 2 ) z = ( D + D ′ ) ( D + 2 D ′ ) z
1 STEP: Let find C.F.
{ ( D + D ′ ) z ( b D − a D ′ − c ) z → { b = 1 a = − 1 c = 0 → ( C . F . ) 1 = e ( 0 ⋅ x 1 ) ⋅ φ 1 ( 1 ⋅ y + ( − 1 ) ⋅ x ) → ( C . F . ) 1 = φ 1 ( y − x ) , where φ 1 is arbitrary function \begin{aligned}
\left\{(D + D')z \atop (bD - aD' - c)z \right. &\rightarrow \left\{ \begin{array}{l} b = 1 \\ a = -1 \\ c = 0 \end{array} \right. \rightarrow (C.F.)_1 = e^{\left(\frac{0 \cdot x}{1}\right)} \cdot \varphi_1(1 \cdot y + (-1) \cdot x) \rightarrow \\
&\quad \boxed{(C.F.)_1 = \varphi_1(y - x), \text{ where } \varphi_1 \text{ is arbitrary function}}
\end{aligned} { ( b D − a D ′ − c ) z ( D + D ′ ) z → ⎩ ⎨ ⎧ b = 1 a = − 1 c = 0 → ( C . F . ) 1 = e ( 1 0 ⋅ x ) ⋅ φ 1 ( 1 ⋅ y + ( − 1 ) ⋅ x ) → ( C . F . ) 1 = φ 1 ( y − x ) , where φ 1 is arbitrary function { ( D + 2 D ′ ) z ( b D − a D ′ − c ) z → { b = 1 a = − 2 c = 0 → ( C . F . ) 2 = e ( 0 ⋅ x 1 ) ⋅ φ 2 ( 1 ⋅ y + ( − 2 ) ⋅ x ) → ( C . F . ) 2 = φ 2 ( y − 2 x ) , where φ 2 is arbitrary function \begin{aligned}
\left\{(D + 2D')z \atop (bD - aD' - c)z \right. &\rightarrow \left\{ \begin{array}{l} b = 1 \\ a = -2 \\ c = 0 \end{array} \right. \rightarrow (C.F.)_2 = e^{\left(\frac{0 \cdot x}{1}\right)} \cdot \varphi_2(1 \cdot y + (-2) \cdot x) \rightarrow \\
&\quad \boxed{(C.F.)_2 = \varphi_2(y - 2x), \text{ where } \varphi_2 \text{ is arbitrary function}}
\end{aligned} { ( b D − a D ′ − c ) z ( D + 2 D ′ ) z → ⎩ ⎨ ⎧ b = 1 a = − 2 c = 0 → ( C . F . ) 2 = e ( 1 0 ⋅ x ) ⋅ φ 2 ( 1 ⋅ y + ( − 2 ) ⋅ x ) → ( C . F . ) 2 = φ 2 ( y − 2 x ) , where φ 2 is arbitrary function
Then,
C . F . = ( C . F . ) 1 + ( C . F . ) 2 → C . F . = φ 1 ( y − x ) + φ 2 ( y − 2 x ) C.F. = (C.F.)_1 + (C.F.)_2 \rightarrow \boxed{C.F. = \varphi_1(y - x) + \varphi_2(y - 2x)} C . F . = ( C . F . ) 1 + ( C . F . ) 2 → C . F . = φ 1 ( y − x ) + φ 2 ( y − 2 x )
2 STEP: Let find P.I.
P . I . = 1 ( D + D ′ ) ( D + 2 D ′ ) ( 12 x y ) = 1 D ( 1 + D ′ D ) D ( 1 + 2 D ′ D ) ( 12 x y ) = P.I. = \frac{1}{(D + D')(D + 2D')} (12xy) = \frac{1}{D\left(1 + \frac{D'}{D}\right)D\left(1 + \frac{2D'}{D}\right)} (12xy) = P . I . = ( D + D ′ ) ( D + 2 D ′ ) 1 ( 12 x y ) = D ( 1 + D D ′ ) D ( 1 + D 2 D ′ ) 1 ( 12 x y ) = = 1 D 2 ⋅ [ 1 + D ′ D ] − 1 [ 1 + 2 D ′ D ] − 1 ( 12 x y ) = [ 1 1 + x = 1 − x + x 2 − x 3 + x 4 + ⋯ , ∣ x ∣ < 1 ] = = 1 D 2 ⋅ [ 1 − D ′ D + ⋯ ] [ 1 − 2 D ′ D + ⋯ ] ( 12 x y ) = = 1 D 2 ⋅ [ 1 − D ′ D − 2 D ′ D + 2 D ′ 2 D 2 ⋯ ] ( 12 x y ) = 1 D 2 ⋅ [ 1 − 3 D ′ D + 2 D ′ 2 D 2 ⋯ ] ( 12 x y ) = = 1 D 2 ⋅ [ 12 x y − 3 D ⋅ ( ∂ ∂ y ( 12 x y ) ) + 2 D 2 ⋅ ( ∂ 2 ∂ y 2 ( 12 x y ) ) + ⋯ ] = = [ 1 D ≡ ∫ d x ] = 1 D 2 ⋅ [ 12 x y − 3 D ⋅ 12 x + 2 D 2 ⋅ 0 + ⋯ ] = 1 D 2 ⋅ [ 12 x y − ( 3 ⋅ 12 ) ⋅ ∫ x d x ] = = 1 D 2 ⋅ [ 12 x y − 36 ⋅ x 2 2 ] = 1 D ⋅ ( ∫ ( 12 x y − 18 x 2 ) d x ) = 1 D ⋅ ( 12 y x 2 2 − 18 x 3 3 ) = = 1 D ⋅ ( 6 y x 2 − 6 x 3 ) = ∫ ( 6 y x 2 − 6 x 3 ) d x = 6 y x 3 3 − 6 x 4 4 = 2 y x 3 − 3 x 4 2 \begin{aligned}
& = \frac{1}{D^{2}} \cdot \left[ 1 + \frac{D'}{D} \right]^{-1} \left[ 1 + \frac{2D'}{D} \right]^{-1} (12xy) = \left[ \frac{1}{1 + x} = 1 - x + x^{2} - x^{3} + x^{4} + \cdots, |x| < 1 \right] = \\
& = \frac{1}{D^{2}} \cdot \left[ 1 - \frac{D'}{D} + \cdots \right] \left[ 1 - \frac{2D'}{D} + \cdots \right] (12xy) = \\
& = \frac{1}{D^{2}} \cdot \left[ 1 - \frac{D'}{D} - \frac{2D'}{D} + \frac{2D'^{2}}{D^{2}} \cdots \right] (12xy) = \frac{1}{D^{2}} \cdot \left[ 1 - \frac{3D'}{D} + \frac{2D'^{2}}{D^{2}} \cdots \right] (12xy) = \\
& = \frac{1}{D^{2}} \cdot \left[ 12xy - \frac{3}{D} \cdot \left(\frac{\partial}{\partial y} (12xy)\right) + \frac{2}{D^{2}} \cdot \left(\frac{\partial^{2}}{\partial y^{2}} (12xy)\right) + \cdots \right] = \\
& = \left[ \frac{1}{D} \equiv \int dx \right] = \frac{1}{D^{2}} \cdot \left[ 12xy - \frac{3}{D} \cdot 12x + \frac{2}{D^{2}} \cdot 0 + \cdots \right] = \frac{1}{D^{2}} \cdot \left[ 12xy - (3 \cdot 12) \cdot \int x \, dx \right] = \\
& = \frac{1}{D^{2}} \cdot \left[ 12xy - 36 \cdot \frac{x^{2}}{2} \right] = \frac{1}{D} \cdot \left( \int (12xy - 18x^{2}) \, dx \right) = \frac{1}{D} \cdot \left( \frac{12yx^{2}}{2} - \frac{18x^{3}}{3} \right) = \\
& = \frac{1}{D} \cdot (6yx^{2} - 6x^{3}) = \int (6yx^{2} - 6x^{3}) \, dx = \frac{6yx^{3}}{3} - \frac{6x^{4}}{4} = 2yx^{3} - \frac{3x^{4}}{2}
\end{aligned} = D 2 1 ⋅ [ 1 + D D ′ ] − 1 [ 1 + D 2 D ′ ] − 1 ( 12 x y ) = [ 1 + x 1 = 1 − x + x 2 − x 3 + x 4 + ⋯ , ∣ x ∣ < 1 ] = = D 2 1 ⋅ [ 1 − D D ′ + ⋯ ] [ 1 − D 2 D ′ + ⋯ ] ( 12 x y ) = = D 2 1 ⋅ [ 1 − D D ′ − D 2 D ′ + D 2 2 D ′ 2 ⋯ ] ( 12 x y ) = D 2 1 ⋅ [ 1 − D 3 D ′ + D 2 2 D ′ 2 ⋯ ] ( 12 x y ) = = D 2 1 ⋅ [ 12 x y − D 3 ⋅ ( ∂ y ∂ ( 12 x y ) ) + D 2 2 ⋅ ( ∂ y 2 ∂ 2 ( 12 x y ) ) + ⋯ ] = = [ D 1 ≡ ∫ d x ] = D 2 1 ⋅ [ 12 x y − D 3 ⋅ 12 x + D 2 2 ⋅ 0 + ⋯ ] = D 2 1 ⋅ [ 12 x y − ( 3 ⋅ 12 ) ⋅ ∫ x d x ] = = D 2 1 ⋅ [ 12 x y − 36 ⋅ 2 x 2 ] = D 1 ⋅ ( ∫ ( 12 x y − 18 x 2 ) d x ) = D 1 ⋅ ( 2 12 y x 2 − 3 18 x 3 ) = = D 1 ⋅ ( 6 y x 2 − 6 x 3 ) = ∫ ( 6 y x 2 − 6 x 3 ) d x = 3 6 y x 3 − 4 6 x 4 = 2 y x 3 − 2 3 x 4
Then,
P . I . = 2 y x 3 − 3 x 4 2 \boxed{P.I. = 2yx^{3} - \frac{3x^{4}}{2}} P . I . = 2 y x 3 − 2 3 x 4
Conclusion,
z ( x , y ) = C . F . + P . I . = φ 1 ( y − x ) + φ 2 ( y − 2 x ) + 2 y x 3 − 3 x 4 2 z(x, y) = C.F. + P.I. = \varphi_{1}(y - x) + \varphi_{2}(y - 2x) + 2yx^{3} - \frac{3x^{4}}{2} z ( x , y ) = C . F . + P . I . = φ 1 ( y − x ) + φ 2 ( y − 2 x ) + 2 y x 3 − 2 3 x 4 { z ( x , y ) = φ 1 ( y − x ) + φ 2 ( y − 2 x ) + 2 y x 3 − 3 x 4 2 where φ 1 and φ 2 are arbitrary functions \boxed{\begin{cases} z(x, y) = \varphi_{1}(y - x) + \varphi_{2}(y - 2x) + 2yx^{3} - \frac{3x^{4}}{2} \\ \text{where } \varphi_{1} \text{ and } \varphi_{2} \text{ are arbitrary functions} \end{cases}} { z ( x , y ) = φ 1 ( y − x ) + φ 2 ( y − 2 x ) + 2 y x 3 − 2 3 x 4 where φ 1 and φ 2 are arbitrary functions
ANSWER: { z ( x , y ) = φ 1 ( y − x ) + φ 2 ( y − 2 x ) + 2 y x 3 − 3 x 4 2 where φ 1 and φ 2 are arbitrary functions \begin{cases} z(x, y) = \varphi_{1}(y - x) + \varphi_{2}(y - 2x) + 2yx^{3} - \frac{3x^{4}}{2} \\ \text{where } \varphi_{1} \text{ and } \varphi_{2} \text{ are arbitrary functions} \end{cases} { z ( x , y ) = φ 1 ( y − x ) + φ 2 ( y − 2 x ) + 2 y x 3 − 2 3 x 4 where φ 1 and φ 2 are arbitrary functions
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