In Proposition III.7 (see also modern version), Euclid shows that in the diagram below $FA > FB > FC > FG > FE$.
Assuming $\angle CFE = \alpha$, what is the actual length of $FC$ (in terms of $FD$) on a unit circle? I tried to determine this algebraically but was not able to (some attempts are here, here, and here, abbreviating $u = FD$).
I also tried to solve geometrically using Power of the Point (again, letting $u = FD$ and $C'$ be the other intersection of $FC$ with the circle): $$(1+u)(1-u) = FC \cdot FC' \\ FC + FC' = ? $$ but could not express $CC'$ in terms of $\alpha$ (or anything else useful).

Letting $u=DF, v=CF, \alpha = \angle CFE, \alpha' = \angle CFD, \beta = \angle CDF, \gamma = \angle DCF$, and noting that $CD = 1$ because it is a radius of the circle, we can use the law of sines to set up two equations of two unknowns:
$$\frac{\sin{\alpha'}}{1} = \frac{\sin{\beta}}{v} = \frac{\sin{\gamma}}{u}$$
Note that $\beta = \alpha - \gamma$ so:
$$\sin{\alpha'} = \frac{\sin{\alpha - \gamma}}{v} = \frac{\sin{\gamma}}{u}$$
Thus $\gamma = \arcsin{(u\sin{\alpha'})}$. Recognize that $\sin{(\alpha - \gamma)} = \sin{\alpha}\cos{\gamma} - \sin{\gamma}\cos{\alpha}$ so:
$$\sin{\alpha'} = \frac{\sin{\alpha}\cos{\gamma} - \cos{\alpha}\sin{\gamma}}{v}$$
Next we realize that $\cos{\gamma} = \sqrt{1 - u^2\sin{\alpha'}}$ and $\sin{\gamma} = u\sin{\alpha'}$ so we end up with:
$$\sin{\alpha'} = \frac{\sin{\alpha}\sqrt{1 - u^2\sin^2{\alpha'}} - u\cos{\alpha}\sin{\alpha'}}{v}$$
Which, solving for $v$ and simplifying, gives us:
$$v = CF = \sin{\alpha}\sqrt{\frac{1}{\sin^2{\alpha'}} - u^2}-u\cos{\alpha}$$
The following plot compares the simulated distance CF as well as the calculated distance using the derived formula (setting $u=0.2$).
Plot of calculated CF distance and simulated distance against $\alpha$
The following Python code produced that plot