(c) r cosec α/2 sin β

Let O be the centre of the balloon of radius r and E the position of the eye of the observer.
Let EA, EB be the tangents from E to the balloon.
Then,
∠EAB = α.
Let OL be the perpendicular from O on the horizontal line EX.
Given,
∠OEL = β
∠OLE = 90°,
∠OBE = 90° = ∠OAE (∵ radius \(\perp\) to the tangent at point of contact)
Also,
∠BEO = ∠AEO = \(\frac{\alpha}{2}\) (∵ DAEO ≅ DBEO)
In rt. Δ OAE,
\(sin\frac{\alpha}{2}=\frac{OA}{OE}\)
⇒ OE = OA cosec \(\frac{\alpha}{2}\) = r cosec \(\frac{\alpha}{2}\) ....(i)
In rt. Δ OLE,
sin β = \(\frac{OL}{OE}\)
⇒ OL = OE sin β
= r cosec \(\frac{\alpha}{2}\)sin β [From (i)]