A trigonometric problem when calculating distance to the boundary of a convex hull Suppose we have a sphere and a point outside of the sphere. 
We denote the point outside as $v$ and the origin of the sphere as $x$. The convex hull of the sphere and $v$ should be like an ice cream cone. 
So for a point inside of the convex hull, say $u$, I want to prove that the distance to the boundary of the convex hull can be solved by a reduced problem where we consider only the part of the plane intersecting the convex hull containing points $x, u, v$. 
The reduced problem is illustrated in the figure.
Basically, the question is: Does this restriction to the plane give the shortest distance to the boundary of the convex hull? How can we prove it?
This seems like a trivial fact but it does not seem like that easy to prove...
From any other ray propagated from $v$ on the convex hull, we draw a segment from u perpendicular to it. Let the distance between $v$ and $u$ be $L$, and the angle between $\overline{vu}$ and the two rays be $\alpha$ and $\beta$, respectively. Since $\alpha$ and $\beta$ must be in $(0,\frac{\pi}{2})$, and length of the two distances we need to compare is $L\sin{\alpha}$ and $L\sin{\beta}$. It would suffice just to compare $\alpha$ and $\beta$. But I don't know how to proceed from here.
Any suggestions would be appreciated.

I'm not entirely sure what you mean by the transverse of the convex hull, but assuming this is equivalent to the plane defined by $u$, $v$, and $x$, I believe the following approach leads to a relatively simple proof:
We can find the shortest distance by expanding a sphere outwards from $u$ until it is tangent to some point $t$ (if there are multiple such points, choose one) on the boundary of the cone. That this point of contact is in fact a point of tangency follows from the convexity of the region, I believe. 
Then we know that $\overline{ut}$ will be orthogonal to the plane of tangency at $t$. But we also know that any such lines orthogonal to the region at some $t$ will intersect $\overline{vx}$, from the basic geometry of cones and spheres (by symmetry, all such lines pass through the axis of rotational symmetry of a cone and through the center $x$ for the sphere). From the fact that $\overline{ut}$ and $\overline{vx}$ intersect, we have that they are coplanar, which is what we set out to prove.
