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

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The discussion focuses on solving the partial differential equation (PDE) represented by 3u_x + 4u_y - 2u = 1, leading to the auxiliary condition ω_ξ + kω = φ(ξ, η). The transformation u(x, y) = ω(ξ, η) is established using the relationships u_x and u_y, with specific values for constants A, B, C, and D. The choice of A = 3 and C = 4 simplifies the equation to ω_ξ - 2ω = 1. The arbitrary constants B and D are determined to satisfy the auxiliary condition u(x, 0) = u_0(x), with D set to 0 and B chosen as 1.

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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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