Line charge density expressed via Dirac delta function

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Heirot
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Homework Statement



Let's say we have a wire of finite length L with total charge Q evenly spread along the wire so that lambda=Q/L, linear charge density, is constant. The wire is shaped in x-y plane in some well behaved curve y = f(x). Find the surface charge density sigma(x,y).

Homework Equations



Q = Int(lambda dl) = Int ( Sqrt(1+(dy/dx)^2) dx) for line charge density
Q = Int(sigma(x,y) dx dy) for surface charge density

The Attempt at a Solution



The most logic thing to do would be to write sigma(x,y) = lambda * delta(y-f(x)), where delta(x) is Dirac's delta function. Unfortunately, this doesn't give the right Q, because integration of the delta function over y only give 1 and not the required Sqrt(1+(dy/dx)^2).

Where's the error in reasoning?
 
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But

[tex] \begin{equation*}<br /> \begin{split}<br /> Q &= \lambda L \\<br /> &= \lambda \int \sqrt{1 + \left( \frac{dy}{dx}\right)^2} dx.<br /> \end{split}<br /> \end{equation*}[/tex]

Heuristically, the amount of charge on the wire between [itex]x[/itex] and [itex]x + dx[/itex] is

[tex]dQ = \lambda dL = \lambda \sqrt{1 + \left( \frac{dy}{dx}\right)^2} dx.[/tex]
 
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I agree. So, dQ = sigma(x,y) dx dy. What's sigma(x,y)?