Question #66041

solve; [D^3 − DD′^2 − D^2 + DD′] z = 0

Expert's answer

Answer on Question 66041 - Math - Differential Equations

Question: Solve

(D3DD2D2+DD)z=0.(D^{3}-DD^{\prime 2}-D^{2}+DD^{\prime})z=0. (1)

Solution: Recall that D=xD=\frac{\partial}{\partial x}, D=yD^{\prime}=\frac{\partial}{\partial y}. We look for the general solution z=z(x,y)z=z(x,y) of the PDE with constant coefficients

3zx33zxy22zx22zxy=0.\frac{\partial^{3}z}{\partial x^{3}}-\frac{\partial^{3}z}{\partial x\partial y^{2}}-\frac{\partial^{2}z}{\partial x^{2}}-\frac{\partial^{2}z}{\partial x\partial y}=0.

This operator is reducible

D3DD2D2+DD=D(DD)(D+D1).D^{3}-DD^{\prime 2}-D^{2}+DD^{\prime}=D(D-D^{\prime})(D+D^{\prime}-1).

Therefore the general solution of (1) has the form [1]

z(x,y)=u(x,y)+v(x,y)+w(x,y),z(x,y)=u(x,y)+v(x,y)+w(x,y),

where uu, vv and ww are general solutions of the first order PDEs

ux=0,vxvy=0,wx+wyw=0u_{x}=0,\qquad v_{x}-v_{y}=0,\qquad w_{x}+w_{y}-w=0

respectively. All these PDEs can be directly solved by the Lagrange method:

ux=0u(x,y)=f(y);u_{x}=0\quad\Rightarrow\quad u(x,y)=f(y);

vxvy=0dx=dyx+y=cv(x,y)=g(x+y);v_{x}-v_{y}=0\quad\Rightarrow\quad dx=-dy\quad\Rightarrow\quad x+y=c\quad\Rightarrow\quad v(x,y)=g(x+y);

wx+wy=wdx=dy=dwwxy=c1,  wex=c2w_{x}+w_{y}=w\quad\Rightarrow\quad dx=dy=\frac{dw}{w}\quad\Rightarrow\quad x-y=c_{1},\;we^{-x}=c_{2}

wex=h(xy)w=exh(xy),\quad\Rightarrow\quad we^{-x}=h(x-y)\quad\Rightarrow\quad w=e^{x}h(x-y),

where ff, gg and hh are arbitrary C1C^{1}-functions. Finally,

z(x,y)=f(y)+g(x+y)+exh(xy).z(x,y)=f(y)+g(x+y)+e^{x}h(x-y).

Answer: z(x,y)=f(y)+g(x+y)+exh(xy)z(x,y)=f(y)+g(x+y)+e^{x}h(x-y), where ff, gg and hh are arbitrary C1C^{1}-functions.

References

- [1] Sneddon, Ian N., and J. C. Polkinghorne. Elements of partial differential equations. Physics Today 10.5 (1957): 96–109.


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