I have the following problem: Find the solution for $\Delta u = 0$ for which $u(\cos(t), \sin(t)) = t(2\pi - t), \\ 0 \leq t \leq 2\pi$.
My attempt:
I rewrite $u(\cos(t), \sin(t)) = u(x(t), y(t))$ with $x(t) = \cos(t), \ y(t) = \sin(t)$. The Laplace equation is $\frac{d^2 u}{dx^2} + \frac{d^2 u}{dy^2} = 0$, where $\frac{d^2 u}{dx^2} = \frac{d}{dx} (\frac{du}{dx})$ and $\frac{d^2 u}{dy^2} = \frac{d}{dy} (\frac{du}{dy})$. Since $x(t) = \cos(t), \ y(t) = \sin(t)$, $u$ is basically a function of $t$, so I use the chain rule to get $\frac{du}{dt} = \frac{\partial u}{\partial x} \frac{dx}{dt} + \frac{\partial u}{\partial y} \frac{dy}{dt}$.
So we have $\frac{dx}{dt} = \frac{d}{dt} \cos(t) = -\sin(t)$ and $\frac{dy}{dt} = \frac{d}{dt} \sin(t) = \cos(t)$. Here I run into some problems.
- How do I calculate $\frac{\partial u}{\partial x}$ and $\frac{\partial u}{\partial y}$ ?
Because, as far as I understand it, I should rewrite the part $t(2\pi - t)$ in terms of $x$ and $y$ (or maybe in terms of $\cos(t)$ and $\sin(t)$ ?). But I don't know how to do it (if it's even necessary)
- How would the Laplace equation then look in terms of $u$ being dependent on $t$?
Try this:
$$\frac{d}{dx}(*)=\frac{\frac{d}{dt}(*)}{\frac{dx}{dt}}$$ $$\frac{du}{dx}=\frac{\frac{du}{dt}}{\frac{dx}{dt}}=\frac{\frac{d}{dt}[t(2\pi-t)]}{\frac{d}{dt}[cos(t)]}=\frac{2\pi-2t}{-sin(t)}$$
If you need $\frac{d}{dx}(\frac{du}{dx})$then reapply the first formula.
UPDATE:
The plan is to write the expression of function u not in terms of t but in terms of x and y.
Step1: process the equation ${\Delta u=0}$ to a form similar to $tan^2(t)+2(\pi-t)\cdot tan(t)+1=0$ This equation is an example, please do your own work!
Step 2: solve for t as a dependency of $tan(t)$
Step 3: replace $tan(t)=\frac{sin(t)}{cos(t)}=\frac{y}{x}$ and find $t(x,y)$
Step 4: rewrite $u(x,y)=t(2\pi-t)$, where $t=t(x,y)$ previously determined
Step 5: rewrite $\Delta u=0$ only in terms of x and y