The velocity of a small ball of mass M and density d, when dropped in a container filled with glycerin becomes constant after some time. If the density of glycerin is $\frac {d}{2}$, then the viscous force acting on the ball will be:
(1) $\frac {Mg}{2}$
(2) $Mg$
(2) $Mg$
(3) $\frac {3}{2} Mg$
(4) $2Mg$
Solution
When velocity is constant, net force = 0.
$\therefore B+F=Mg$
Since density of glycerin is $\frac {1}{2}$ of the density of the ball, the buoyant force is half of the weight of the ball.
$B=\frac {Mg}{2}$
Now, $\frac {Mg}{2}+F=Mg$
$\therefore F=\frac {Mg}{2}$
Answer: (1)