Finding Auxiliary Conditions for u(x,y) and Solving for ω(ξ,η)

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Homework Help Overview

The discussion revolves around finding auxiliary conditions for a function u(x,y) and solving for ω(ξ,η) in the context of a partial differential equation. The problem involves transforming variables and deriving relationships between derivatives of the functions involved.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the transformation of variables and the implications of choosing constants A, B, C, and D. There is an exploration of how these choices affect the derived equations and the understanding of the auxiliary conditions.

Discussion Status

Some participants express understanding of the initial transformations and equations, while others seek clarification on specific choices of constants and their implications for the auxiliary conditions. There is an ongoing exploration of the relationships between the variables and the conditions that must be satisfied.

Contextual Notes

Participants note that the choice of constants B and D is arbitrary, with the requirement that AD - BC ≠ 0. There is a specific focus on aligning the auxiliary condition with the prescribed data at y = 0.

Dustinsfl
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2.2.2 3u_x+4u_y-2u=1\Rightarrow \omega_{\xi}+k\omega=\varphi(\xi,\eta)

u(x,y)=u(\xi\cos{\alpha}-\eta\sin{\alpha},\xi\sin{\alpha}+\eta\cos{\alpha})=\omega(\xi,\eta)

u_x=\omega_{\xi}\cos{\alpha}-\omega_{\eta}\sin{\alpha}

u_y=\omega_{\xi}\sin{\alpha}+\omega_{\eta}\cos{\alpha}

3(\omega_{\xi}\cos{\alpha}-\omega_{\eta}\sin{\alpha})+4(\omega_{\xi}\sin{\alpha}+\omega_{\eta}\cos{\alpha})-2w=1

\omega_{\xi}(3\cos{\alpha}+4\sin{\alpha})+\omega_{\eta}(4\cos{\alpha}-3\sin{\alpha})-2\omega=1

\displaystyle 4\cos{\alpha}-3\sin{\alpha}=0\Rightarrow \tan{\alpha}=\frac{4}{3}

We have a 3,4,5 right triangle.

\displaystyle\cos{\alpha}=\frac{3}{5} \ \mbox{and} \ \sin{\alpha}=\frac{4}{5}

Substitution:

\displaystyle \omega_{\xi}\left(3\frac{3}{5}+4\frac{4}{5}\right)+\omega_{\eta}(0)-2\omega=1

\displaystyle \omega_{\xi}\left(\frac{9+16}{5}\right)-2\omega=1\Rightarrow\omega_{\xi}-\frac{2}{5}\omega=1

I understand everything posted above; however, I don't understanding anything below.

Let

2.2.8 x=A\xi+B\eta \ \mbox{and} \ y=C\xi+D\eta

A,B,C,D are constants to be determined, and set u(x,y)=\omega(\xi,\eta) 2.2.9

Then, from \displaystyle\frac{\partial\omega}{\partial\xi}=u_x\frac{\partial x}{\partial\xi}+u_y\frac{\partial y}{\partial\xi} and 2.2.8, 2.2.9, we see that with the choice A = 3, C = 4, Equation 2.2.2 becomes \omega_{\xi}-2\omega=1(nope don't see it).
 
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Dustinsfl said:
2.2.2 3u_x+4u_y-2u=1\Rightarrow \omega_{\xi}+k\omega=\varphi(\xi,\eta)

...

Let

2.2.8 x=A\xi+B\eta \ \mbox{and} \ y=C\xi+D\eta

A,B,C,D are constants to be determined, and set u(x,y)=\omega(\xi,\eta) 2.2.9

Then, from \displaystyle\frac{\partial\omega}{\partial\xi}=u_x\frac{\partial x}{\partial\xi}+u_y\frac{\partial y}{\partial\xi} and 2.2.8, 2.2.9, we see that with the choice A = 3, C = 4, Equation 2.2.2 becomes \omega_{\xi}-2\omega=1(nope don't see it).
I didn't read any of the stuff that I didn't include in the quote, but it doesn't look like we need it. Do you realize that \partial x/\partial \xi=A and so on? So

\omega_\xi=\frac{\partial\omega}{\partial\xi}=Au_x+Cu_y=3u_x+4u_y

and you're almost done.
 


Yes, I understand. Thank you.
 


I have a follow-up question now though.

The choice for B and D is arbitrary, except that AD - BC\neq 0.

Looking ahead to the effort to satisfy the auxiliary condition u(x,0)=u_0(x), we shall choose B and D so that the line \xi=0 is the line on which the auxiliary data is prescribed, namely y = 0. This requires D = 0, and, since B is arbitrary we make the convenient choice B = 1.

Can you explain this?
 

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