jedishrfu said:
Yes, we'd be curious how you came up with the equation.
Ok. I was reading about
Hausdorff dimension, and I wanted to find a continuous, compact surface, without holes, with dimension [itex]1 \leq r \leq 2[/itex].
So, the area function A(x), to have a Hausdorff dimension r, must satisfy this equation: [itex]\epsilon A_{(\frac{x}{\epsilon})} = \epsilon^r A_{(x)}[/itex].
Equivalently:
[itex]A_{(\frac{x}{\epsilon})} = \epsilon^{r-1} A_{(x)}[/itex] [
I]
The derivative of A(x) is
[itex]A'_{(x)}=\lim_{\epsilon \to 1}\frac{A_{(x.\epsilon)}-A_{(x)}}{x.\epsilon-x}[/itex] [
II]
Because [
I]
[itex]A_{(x.\epsilon)}=\epsilon^{1-r} A_{(x)}[/itex]
So [
II] is
[itex]A'_{(x)}=A_{(x)} \lim_{\epsilon \to 1}\frac{\epsilon^{1-r}-1}{x.\epsilon-x} = A_{(x)} \frac{1-r}{x}[/itex]
Solving it: [itex]A_{(x)}=c_1 x^{(1-r)}[/itex]
I think that is the only solution for [
I], but do not have proof.
I now want this area to continuously transform from the real line (dimension r=1) to the complex plane (r=2), so I want a 2D surface curved in 3D space with area A(x).
I want to find the function radius R(x) whose
surface of revolution is A(x).
My equation is [itex]A_x =2\pi \int R_{(x)} \sqrt{1+\left( R'_{(x)}\right)^2} \, dx[/itex] [
IV]
I will deal with integration limits later.
Deriving [
IV] and squaring both sides, I get:
[itex]\left (\frac {c_1 (1-r)}{2 \pi} \right)^2 x^{-2r} = R_{(x)} ^2 + \left ( R_{(x)} R'_{(x)} \right )^2[/itex]
Replacing
[itex]R_{(x)}^2 =2y[/itex]
[itex]R_{(x)}R'_{(x)} =y'[/itex]
[itex]a= - \left (\frac {c_1 (1-r)}{2 \pi} \right)^2[/itex]
[itex]b= - 2r[/itex]
I get the differential equation I want to solve:
[itex]2y + y'^2 + a x^b=0[/itex]
I had been vaguely told that should look on
Weierstrass[/PLAIN] p function, [itex]\wp[/itex] and that it may have a closed solution for [itex]b \in \mathbb{Z}[/itex].
I found
this paper, about using the [itex]\wp[/itex] function for solving differential equations, but I can't figure how to use it.