Solving Klein-Gordon PDE w/ Change of Variables

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    Klein-gordon Pde
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Discussion Overview

The discussion revolves around the solution of the Klein-Gordon partial differential equation (PDE) using a change of variables. Participants explore the transformation of the equation and the derivation of boundary conditions resulting from this transformation.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • One participant presents the original Klein-Gordon PDE and the proposed change of variables, expressing confusion about the derivation of the boundary conditions.
  • Another participant suggests checking the definitions of the variables to understand how the boundary conditions are transformed, specifically noting that when y=0, it leads to xi=eta.
  • A subsequent reply confirms that it is valid to express the boundary condition as G(eta,eta)=0, indicating agreement with the previous explanation.

Areas of Agreement / Disagreement

Participants generally agree on the transformation process and the implications for the boundary conditions, but the initial understanding of the boundary conditions remains a point of clarification rather than outright consensus.

Contextual Notes

The discussion does not resolve all aspects of the transformation or the implications of the boundary conditions, leaving some assumptions and interpretations open to further exploration.

yonatan
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Hi.
I'm following the solution of a Klein-Gordon PDE in a textbook. The equation is
\begin{align}<br /> k_{xx}(x,y) - k_{yy}(x,y) &amp;= \lambda k(x,y) \\<br /> k(x,0) &amp;= 0 \\<br /> k(x,x) &amp;= - \frac{\lambda}{2} x<br /> \end{align}<br />
The book uses a change of variables
$\xi = x+y$, $\eta = x-y$
to write
\begin{align}<br /> k(x,y) &amp;= G(\xi,\eta)\\<br /> k_{xx} &amp;= G_{\xi \xi} + 2G_{\xi \eta} + G_{\eta \eta}\\<br /> k_{yy} &amp;= G_{\xi \xi} - 2G_{\xi \eta} + G__{\eta \eta}<br /> \end{align}
and then they write the original PDE as
\begin{align}<br /> G_{\xi \eta}(\xi,\eta) &amp;= \frac{\lambda}{4} G(\xi,\eta),\\<br /> G(\xi,\xi) &amp;= 0,\\<br /> G(\xi,0) &amp;= - \frac{\lambda}{4} \xi<br /> \end{align}<br />
I'm fine with the first line in the new PDE, but the other two, the boundary conditions, i don't get how they arrive at.

Can somebody help me understand? I'll be much appreciative :-)

J.
 
Last edited:
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Basically just check the definition!

k(x,y)=G(xi,eta)

In the first boundary condition, k(x,0)=0.
now what does y=0 mean? xi=x+y and eta=x-y, hence y=0 means: xi=x and eta=x, hence xi=eta, hence k(x,0)=G(xi,xi)=0

similarly for the second one..
 
I see, thanks. Would it then be the same, for the case k(x,0)=0, where y=0 and xi=eta, to write G(eta,eta)=0?
 
Absolutely! :)
 

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