Problems

Solution: The area for \(\alpha\) fixed is \(\frac12 r^2 \sin \alpha + \frac12 r^2 \sin \theta + \frac12 r^2 \sin (\pi - \theta - \alpha)\) So we wish to maximise \(V = \sin \theta + \sin(\pi - \theta-\alpha)\) \begin{align*} && V &= \sin \theta + \sin(\pi - \theta-\alpha)\\ &&&= 2\sin \l \frac{\pi-\alpha}2\r\cos \l \frac{2\theta + \alpha - \pi}{2}\r \end{align*} The largest \(\cos\) can be is \(1\) when \(\displaystyle 2\theta + \alpha - \pi = 0 \Rightarrow \theta = \frac{\pi-\alpha}2\). (ie we split the remaining area exactly in half). We are now trying to maximise \(W = \sin \alpha + 2 \sin \frac{\pi - \alpha}2\) ie \begin{align*} && W &= \sin \alpha + 2 \cos \frac{\alpha}{2} \\ \Rightarrow && \frac{\d W}{\d \alpha} &= \cos \alpha-\sin \frac{\alpha}{2} \\ &&&= 1-2 \sin^2 \frac{\alpha}{2} - \sin \frac{\alpha}{2} \\ &&&= (1+\sin \frac{\alpha}{2})(1-2\sin \frac{\alpha}{2}) \end{align*} Therefore \(\frac{\alpha}{2} = -\frac{3\pi}{2}, \frac{\alpha}{2} = \frac{\pi}{6}, \frac{5\pi}{6} \Rightarrow \alpha = -3\pi, \frac{\pi}{3}, \frac{5\pi}{3}\). The only turning point in our range is \(\frac{\pi}{3}\). This is obvious a a maximum by symmetry or checking the end points, but we could also check the second derivative \(\frac{\d^2 W}{\d \alpha^2} = -\sin \frac{\pi}{3}-\cos \frac{\pi}{3} < 0\) so we have a maximum. Therefore the largest possible area is: \(\displaystyle \frac{3\sqrt{3}}{4}r^2\)