We have two charges separated by a distance \(d\). In air, the force between them is \(F\). When placed in a dielectric medium at the same distance, the force becomes \(F/2\). We need to find the dielectric constant of the medium.
The electrostatic force between two charges \(q_1\) and \(q_2\) separated by a distance \(d\) in a vacuum (or air, which is a good approximation) is given by Coulomb's Law:
\(F = \frac{1}{4\pi\epsilon_0} \frac{|q_1 q_2|}{d^2}\)
Where:
When the charges are placed in a dielectric medium, the electrostatic force is reduced by a factor of the dielectric constant \(K\). Let \(F'\) be the force in the dielectric medium:
\(F' = \frac{1}{4\pi\epsilon_0 K} \frac{|q_1 q_2|}{d^2}\)
Where \(K\) is the dielectric constant (also known as the relative permittivity \(\epsilon_r\)).
We are given that the force in the dielectric medium is \(F/2\):
\(F' = \frac{F}{2}\)
Substitute the expressions for \(F\) and \(F'\):
\(\frac{1}{4\pi\epsilon_0 K} \frac{|q_1 q_2|}{d^2} = \frac{1}{2} \left( \frac{1}{4\pi\epsilon_0} \frac{|q_1 q_2|}{d^2} \right)\)
Notice that the terms \(\frac{1}{4\pi\epsilon_0} \frac{|q_1 q_2|}{d^2}\) appear on both sides, so we can cancel them out:
\(\frac{1}{K} = \frac{1}{2}\)
Solving for \(K\), we get:
\(K = 2\)
The dielectric constant of the medium is 2.
The force between two charges in a medium is given by Coulomb’s law: \[ F_{\text{medium}} = \frac{F_{\text{air}}}{K} \] Where:
\( F_{\text{air}} = F \) is the force in air
\( F_{\text{medium}} = \frac{F}{2} \) is the force in dielectric medium
\( K \) is the dielectric constant of the medium Now substitute the values: \[ \frac{F}{2} = \frac{F}{K} \Rightarrow K = 2 \]