#11: Maxwell's first equation says that the flow of electric fields across the surface of any compact volume is determined entirely by the total charge inside that volume. This means that no matter which closed surface you put around a point charge, the resulting flow is always the same. So if it's 4πq for a small sphere, then it's also 4πq for a dodecahedron.
#15: The area conversion factor for a parametrization t : (u, v) -> (x(u,v), y(u,v), z(u,v)) is given by |tu(u, v) x tv(u,v)| (the cross product of the derivatives by u resp. v). In this case, t(u,v) = (u, v, au+bv+c), therefore tu(u, v) = (1, 0, a) and tv(u, v) = (0, 1, b), therefore tu(u, v) x tv(u, v) = (-a, -b, 1) and the area conversion factor is therefore given by sqrt(a²+b²+1²).
To create the formula, we first need to find the parameter space for that part of the plane. Let's call B the part of the plane with points (x, y, z) satisfying x²+y²<=r², and let's call A the part of the parameter space with points (u, v) satisfying x(u, v)²+y(u, v)²<=r², which by definition of x(u, v) and y(u, v) is equivalent to u²+v²<r².
Now we know that the surface area of B is given by ∫B1ds, which is defined as ∫ASAxyz[u, v]d(u, v) = ∫Asqrt(a²+b²+1²)d(u, v) = sqrt(a²+b²+1²) * ∫A1d(u, v) = sqrt(a²+b²+1²) * (the area of A). We know that A is a circle of radius r, which has the area πr², so the surface of B is exactly sqrt(a²+b²+1)*πr².