Difference between revisions of "Talk:Eigenfunction Matching for a Finite Dock"
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The link for the finite.m file is broken. Or maybe the file doesn't exist yet. | The link for the finite.m file is broken. Or maybe the file doesn't exist yet. | ||
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| + | == Expression of the potential under the dock == | ||
| + | |||
| + | It seems that the eigenfunctions | ||
| + | <math> | ||
| + | \frac{L\pm x}{2L}\psi_{0}(z) | ||
| + | </math> | ||
| + | do not satisfy the Laplace equation. Nor do any linear combination of them so it seems to me that we have to write <math>b_0=c_0=0</math> which means removing them from the potential expression. | ||
Revision as of 15:59, 11 April 2008
Broken link
The link for the finite.m file is broken. Or maybe the file doesn't exist yet.
Expression of the potential under the dock
It seems that the eigenfunctions [math]\displaystyle{ \frac{L\pm x}{2L}\psi_{0}(z) }[/math] do not satisfy the Laplace equation. Nor do any linear combination of them so it seems to me that we have to write [math]\displaystyle{ b_0=c_0=0 }[/math] which means removing them from the potential expression.
