The unrolled surface shown in the above figure is in the form of a sector of a sector with radius L, central angle
θ, and length of arc s. The length of arc s is the circumference of the base of the cone which is denoted by c. Thus s = c.
$c = 2 \pi r$
$s = L \theta_{rad}$
$s = c$
$L \theta_{rad} = 2 \pi r$
$\theta_{rad} = \dfrac{2 \pi r}{L}$
$A_L = A_{sector}$
$A_L = \frac{1}{2} sL$
$A_L = \frac{1}{2}(L \theta_{rad})L$
$A_L = \frac{1}{2} L^2 \theta_{rad}$
$A_L = \frac{1}{2} L^2 \left( \dfrac{2 \pi r}{L} \right)$
$A_L = \pi rL$ (okay!)