Griffith's E&M: Why is V_0(y) Missing from Equation 3.28?

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Griffith's E&M discusses boundary conditions and their implications in solving partial differential equations (PDEs). Specifically, condition III, V=V_0(y) when x=0, raises questions about the absence of V_0(y) in equation 3.28, V(x,y) = Ce^(-ky)sin(ky). The equation provides an infinite set of solutions through the separation ansatz, allowing for any solution to be expressed as an infinite series. Boundary condition III helps define coefficients in this series, leading to a generalized Fourier-series expansion. Understanding this technique is crucial for theoretical physics, as highlighted in Griffiths's textbook.
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Does anyone here have a copy of Griffith's E&M?

On page 128, condition III V=V_0 (y) when x = 0.

Do you know why then value V_0(y) does not appear in in equation 3.28, V(x,y) = Ce^(-ky)sin(ky)?

The author does not explain this.
 
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Have you read the solution to the end carefully? (3.28) gives you an infinite set of solutions given the separation ansatz (3.22), working in the boundary conditions (i) and (ii). Now you can get any solution by an infinite series as explained just in the following paragraphs. Then you can use the boundary condition (iii) to define the corresponding coefficients in the general series, which here is a Fourier series in the narrow sense. The general technique of separation of variables to solve PDEs leads to generalized Fourier-series expansions, which is a very important technique in theoretical physics. You should thus carefully study this (in my opinion very nicely explained) example in Griffiths's textbook!
 
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