Stokes' law & Terminal Velocity is considered one the most difficult concept.
29 Questions around this concept.
Spherical balls of radius are falling in a viscous fluid of viscosity
with a velocity
. The retarding viscous force acting on the spherical ball is:
A spherical solid ball of volume V is made of a material of density 1. It is falling through a liquid of density
2 (
2 <
1). Assume that the liquid applies a viscous force on the ball that is proportional to the square of its speed
. The terminal speed of the ball is
Which of the following options correctly describes the variation of the speed v and acceleration ‘a’ of a point mass falling vertically in a viscous medium that applies a force F =−kv, where ‘k’ is a constant, on the body? (Graphs are schematic and not drawn to scale)
From amongst following curves, which one show the variation of the velocity v with time t for a small-sized spherical body (release from rest) falling vertically downwards in a long column of a viscous liquid is best represented by
If the terminal speed of a sphere of gold is 0.2 m/s in a viscous liquid
, find the terminal speed (in m/sec) of a sphere of silver
of the same size in the same liquid.
When a body moves through a fluid then The fluid exerts a viscous force on the body to oppose its motion.
And according to Stokes' law, the magnitude of the viscous force depends on the shape and size of the body, its speed and the viscosity of the fluid.
So for the below figure

If a sphere of radius $r$ moves with velocity $\vee$ through a fluid of viscosity $\eta$.
Then using Stokes' law the viscous force ( F ) opposing the motion of the sphere is given by
$$
F=6 \pi \eta r v
$$
Where
$$
\eta-\text { coefficient viscosity }
$$
$r-$ radius
$v$ - velocity
When the spherical body is dropped in a viscous fluid, it is first accelerated and then its acceleration becomes zero and it attains a constant velocity and this constant velocity is known as terminal velocity.
For a spherical body of radius r is dropped in a viscous fluid, The forces acting on it are shown in the below figure.

So Forces acting on the body are
1. Weight of Body (W)
$$
W=m g=\frac{4}{3} \pi r^3 \rho g
$$
Where $\rho \rightarrow$ density of body
2. Buoyant/ Thrust Force (T of $F_{B)}$
$$
T=F_B=\frac{4}{3} \pi r^3 \sigma g
$$
where $\sigma \rightarrow$ density of fluid
3. Viscous force ( $F$ )
$$
F=6 \pi \eta r v
$$
So when the body attains terminal velocity the net force acting on the body is zero.
Apply force balance
$$
\begin{aligned}
& F_B+F=W \\
& \rightarrow 6 \pi \eta r v+\frac{4}{3} \pi r^3 \sigma g=\frac{4}{3} \pi r^3 \rho g \\
& \rightarrow 6 \pi \eta r v=\frac{4}{3} \pi r^3 g(\rho-\sigma) \\
& \rightarrow v_t=\frac{2}{9} \frac{r^2(\rho-\sigma)}{\eta} g
\end{aligned}
$$
Where $v_T=$ terminal velocity
From this formula, we can say that
i.e., the Spherical body attains constant velocity in a downward direction.
i.e., the Spherical body attains constant velocity in an upward direction.
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