Delta function and derivative of function wrt itself

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The discussion centers on the expression \(\frac{\partial f(x)}{\partial f(y)} = \delta(x-y)\), which highlights the relationship between a function and its derivative with respect to itself. This expression is interpreted as being equal to 1 when \(x=y\) and 0 otherwise, establishing a broader understanding of manipulations involving the Dirac delta function. Key results are referenced, including integrals involving the delta function that reinforce its properties. The conversation concludes with a reference to Parr and Yang's work in Density Functional Theory, which provides a framework for understanding the functional derivative in this context. Overall, the discussion emphasizes the significance of the Dirac delta function in mathematical expressions and integrals.
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Can someone explain the following profound truth: \frac {\partial f(x)}{\partial f(y)} =\delta(x-y)
 
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The expression \dfrac{\partial f(x)}{\partial g(y)} is really just a short-hand, but there are a handful of rules about which manipulations "usually work" with the short-hand. It turns out that the convention you've named---that \dfrac{\partial f(x)}{\partial f(y)} is 1 if x=y and 0 if x\neq y---gives us a slightly broader notion of "usually".
 
When you see the Dirac delta function in action, you ought to remind yourself:
"How will this look like when I integrate the expression?"

I haven't seen the result you post before, but do remember the two following results:
\int_{-\infty}^{\infty}f(x)\delta{(x-y)}dx=f(y)
\int_{-\infty}^{\infty}f(y)\delta{(x-y)}dy=f(x)
Most likely, your result follows from some clever manipulation of these two basic results.
 
Thanks for the replies.
Have found the answer in Parr and Yang's book on Density Functional Theory:
For a functional F=F[f] have
\delta F = \int \frac {\delta F} {\delta f(y)} \delta f(y) \,dy
In a special case that F=F(f), i.e. F is just some function of f it is required that:
\frac {\delta F(f(x))} {\delta f(y)} = \frac {dF}{df} \delta(x-y) in order to have:
\delta F = \int \frac {\delta F} {\delta f(y)} \delta f(y) \,dx = \frac {dF} {df} \delta f(x)
So that taking F = f, get:
\frac {\delta f(x)} {\delta f(y)} = \delta (x-y)
 
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Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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