Surface integral to line integral

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dspch11
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I am agonizing about the following integral identity:

[tex] \frac{d}{dt} \int \int_{g(x,y) \leq t} f(x,y) dx dy = \int_{g(x,y)=t} f(x,y) \frac{1}{\left| \nabla g(x,y) \right|} ds,[/tex]

where ds is the line element. Clearly, using the Heavisite step function, the condition [tex]g(x,y) \leq t[/tex] is transferred into the integrand. Differentiation with respect to t yields a Dirac delta-function. However, how can I eventually arrive at the line integral. The picture is quite clear, if one imagines a domain defined by [tex]g(x,y) \leq t[/tex] which is growing with t. The increase in the integral can then be evaluated by summing contributions along its circumference with [tex]\left| \nabla g(x,y) \right|[/tex] giving the density of isolines.

How can one formally obtain this result?

Thank you for you help,
Daniel
 
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tiny-tim said:
Have you tried changing variables from x and y to s and g ?

Is this what you suggest:

[tex] s = \int \sqrt{ 1 + (\frac{dy}{dx})^2} dx[/tex]

for constant g we have furthermore:

[tex] g(x,y) = t = const \Rightarrow<br /> g_x + g_y \frac{dy}{dx} = 0[/tex]

and, thus,

[tex] s = \int \sqrt{ 1 + (g_x/g_y)^2} dx[/tex]

The jacobian determinant is

[tex] J = 1/(\left| g_x s_y - g_y s_x \right|) = 1/(\left| 0 - g_y \sqrt{ 1 + (g_x/g_y)^2} \right|) = 1/(\left|\nabla g \right|)[/tex]

What about if [tex]\frac{dy}{dx}[/tex] goes to infinity?