At terminal velocity, the net force on the ball is zero. This implies the viscous drag force \( F_d \) equals the ball's weight: \[ F_d = Mg \] For an object in a viscous medium, drag force is described by Stokes' law: \[ F_d = 6 \pi \eta r v \] where \( \eta \) is the medium's viscosity, \( r \) is the ball's radius, and \( v \) is the velocity. Velocity stabilizes when gravitational force is counteracted by viscous force. Given the glycerine's density is half the ball's, the drag force \( F_d \) at terminal velocity matches the ball's weight, \( Mg \). Consequently, the viscous force on the ball is \( Mg \), leading to the correct answer \( \boxed{Mg} \).