Solveeit Logo

Question

Question: Two identical balls each having mass density \(\rho \), mass \(m\) and charge \(q\) are suspended fr...

Two identical balls each having mass density ρ\rho , mass mm and charge qq are suspended from a common point by two insulating massless strings of angle θ\theta with the vertical. Now both the balls are immersed in a liquid. At equilibrium, θ\theta remains the same. If the mass density of the liquid is σ\sigma then the dielectric constant of liquid will be
a. σρσ\dfrac{\sigma }{{\rho - \sigma }}
b. ρρσ\dfrac{\rho }{{\rho - \sigma }}
c. σρ\dfrac{\sigma }{\rho }
d. ρσ\dfrac{\rho }{\sigma }

Explanation

Solution

To solve this question first we have to draw a proper diagram and then we will proceed further by equating the forces applied on the ball with the help of the diagram. We will use the concept of trigonometry along with the concept of electrostatics.

Formula used:
w=mgw = mg ,
Upthrust =Vσg= V\sigma g ,
V=mρV = \dfrac{m}{\rho }
where mm = mass of the ball,
gg = acceleration due to gravity,
VV = volume of the submerged portion,
σ\sigma = density of liquid,
ρ\rho = density of the ball.

Complete step by step answer:

Initially, the forces acting on each ball are
- Tension
- Weight
The electrostatic force of repulsion FF for its equilibrium along vertical, where θ\theta is the angle made by the string and the vertical
Tcosθ=mgT\cos \theta = mg ........ (1)\left( 1 \right)
And along horizontal, we have
Tsinθ=FT\sin \theta = F ......... (2)\left( 2 \right)
Dividing equation (2)\left( 2 \right) by (1)\left( 1 \right) , we get
TsinθTcosθ=Fmg\dfrac{{T\sin \theta }}{{T\cos \theta }} = \dfrac{F}{{mg}}
On further solving we get,
sinθcosθ=Fmg\dfrac{{\sin \theta }}{{\cos \theta }} = \dfrac{F}{{mg}}
tanθ=Fmg\Rightarrow \tan \theta = \dfrac{F}{{mg}} ........... (3)\left( 3 \right)

Now, when the balls are suspended in a liquid of density σ\sigma and dielectric constant KK , the electrostatic force will become 1K\dfrac{1}{K} times, i.e.
F=FKF' = \dfrac{F}{K}
While weight becomes original weight-upthrust.
But before that, let us know Upthrust, which can be defined as the upward force applied by a liquid on an object immersed (partially or fully) or floating in the liquid
Mathematically it can be written as
Upthrust=VσgUpthrust = V\sigma g .
This is also known as the buoyant force.
mg=mgUpthrustmg' = mg - \text{Upthrust}
mg=mgVσg\Rightarrow mg' = mg - V\sigma g
As we know, V=mρV = \dfrac{m}{\rho }

Therefore, mg=mg(mρ)σgmg' = mg - \left( {\dfrac{m}{\rho }} \right)\sigma g
Taking mgmg as common, we get
mg=mg[1σρ]mg' = mg\left[ {1 - \dfrac{\sigma }{\rho }} \right] ............ (4)\left( 4 \right)
Now, for the equilibrium of the balls, we need a relation between the new or apparent force and the apparent weight, given as below
F=mgtanθF' = mg'\tan \theta ' ............. (5)\left( 5 \right)
Angle changes from θ\theta to θ\theta ' because of the apparent force applied
Now, let us substitute the value of mgmg' from the equation (4)\left( 4 \right) in equation (5)\left( 5 \right)

So we get:
F=mg[1σρ]tanθF' = mg\left[ {1 - \dfrac{\sigma }{\rho }} \right]\tan \theta '
Let us find the value of tanθ\tan \theta ' from the above equation:
tanθ=Fmg[1σρ]\tan \theta ' = \dfrac{{F'}}{{mg\left[ {1 - \dfrac{\sigma }{\rho }} \right]}}
And we know F=FKF' = \dfrac{F}{K}
tanθ=FKmg[1σρ]\tan \theta = \dfrac{{\dfrac{F}{K}}}{{mg\left[ {1 - \dfrac{\sigma }{\rho }} \right]}}
tanθ=FKmg[1σρ]\Rightarrow \tan \theta ' = \dfrac{F}{{Kmg\left[ {1 - \dfrac{\sigma }{\rho }} \right]}} ............ (6)\left( 6 \right)
As we know from the given problem statement:
θ=θ\theta = \theta '
tanθ=tanθ\Rightarrow \tan \theta = \tan \theta '
Now, from equation (6)\left( 6 \right) and equation (3)\left( 3 \right) , we have
tanθ=tanθ\tan \theta = \tan \theta '
Fmg=FKmg[1σρ]\Rightarrow \dfrac{F}{{mg}} = \dfrac{F}{{Kmg\left[ {1 - \dfrac{\sigma }{\rho }} \right]}}

Let us now solve this equation to find the value of the dielectric constant KK .
Fmg=FKmg[1σρ]\dfrac{F}{{mg}} = \dfrac{F}{{Kmg\left[ {1 - \dfrac{\sigma }{\rho }} \right]}}
K=mgmg[1σρ]\Rightarrow K = \dfrac{{mg}}{{mg\left[ {1 - \dfrac{\sigma }{\rho }} \right]}}
On further simplifying the equation we get,
K=1[ρσρ]K = \dfrac{1}{{\left[ {\dfrac{{\rho - \sigma }}{\rho }} \right]}}
K=ρρσ\Rightarrow K = \dfrac{\rho }{{\rho - \sigma }}
Thus, the dielectric constant of the liquid is ρρσ\dfrac{\rho }{{\rho - \sigma }}

Hence, the correct answer is option (B).

Note: The relative permittivity of a substance, or dielectric constant, is its permittivity expressed as a ratio to the permittivity of the vacuum. Permittivity is a material property that has an effect on the Coulomb force in the material between two point charges. Two or more solid objects in touch are exerting forces on one another.