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Question: The terminal speed of a sphere of gold (density = \(19.5kg/{m^3}\)) is \(0.2m/s\) in a viscous liqui...

The terminal speed of a sphere of gold (density = 19.5kg/m319.5kg/{m^3}) is 0.2m/s0.2m/s in a viscous liquid (density= 1.5kg/m31.5kg/{m^3}), find the terminal speed of a sphere of silver (density = 10.5kg/m310.5kg/{m^3}) of the same size in the same liquid
A. 0.4m/s
B. 0.133m/s
C. 0.1 m/s
D. 0.2m/s

Explanation

Solution

Hint: The terminal velocity of a body is the speed at which the viscous force and buoyant force together balance its weight so that no net force acts on the body. The relation for terminal velocity is v=29(σρ)r2gηv = \dfrac{2}{9}\dfrac{{(\sigma - \rho ){r^2}g}}{\eta }

Complete step-by-step answer:
We know that when a sphere moves with a velocity vv through a medium of viscosity η\eta , It experiences an opposing Force given by
F=6πrηvF = 6\pi r\eta v where rr is the radius of the sphere.
The terminal velocity of a body can be obtained by equating this viscous force with the apparent weight of the body in the fluid.
For a body falling downwards in a fluid, The net downward force on the body is:
Weight of body - buoyant force
Fd=mgVρgF_d = mg-V \rho g where ρ\rho is the density of the fluid and VV is the volume of the sphere.
At terminal velocity, this downward force and the upward force due to viscosity balance each other.
So we can equate the forces as: mgVρg=6πηrvmg - V\rho g = 6\pi \eta rv

v=mgVρg6πηrv = \dfrac{{mg - V\rho g}}{{6\pi \eta r}}

We can now replace mm in the equation as VσgV\sigma g where V is the volume of sphere and σ\sigma its density to get:
v=V(σρ)g6πηrv = \dfrac{{V(\sigma - \rho )g}}{{6\pi \eta r}}. (1)
In the question, we are asked to compare the terminal velocities of two spheres of different densities with all other parameters fixed.
So we can say from equation (1) that :
vσρ=constant\dfrac{v}{{\sigma - \rho }} = constant
v1σ1ρ=v2σ2ρ\dfrac{{{v_1}}}{{{\sigma _1} - \rho }} = \dfrac{{{v_2}}}{{{\sigma _2} - \rho }}
Substituting the given values of v1{v_1},v2{v_2}, ρ\rho , σ1{\sigma _1} and σ2{\sigma _2} into the equation gives :
0.219.51.5=v210.51.5\dfrac{{0.2}}{{19.5 - 1.5}} = \dfrac{{{v_2}}}{{10.5 - 1.5}}
v2=0.219.51.5(10.51.5){v_2} = \dfrac{{0.2}}{{19.5 - 1.5}}(10.5 - 1.5)
v2=(0.2)(9)18{v_2} = \dfrac{{(0.2)(9)}}{{18}}
v2=0.1m/s{v_2} = 0.1m/s

This is the required answer.

Note: Be careful while using v=(Vσρ)g6πηrv = \dfrac{{(V\sigma - \rho )g}}{{6\pi \eta r}} for other calculations. The VV in equations is also dependent on rr and hence, terminal velocity is not inversely proportional to rr. We may substitute V=43πr3V = \dfrac{4}{3}\pi {r^3} and obtain a general relation: v=29(σρ)r2gηv = \dfrac{2}{9}\dfrac{{(\sigma - \rho ){r^2}g}}{\eta }