To determine the dielectric constant of mica, we first need to understand the effect of a dielectric material inserted between the plates of a capacitor.
Initially, a parallel plate capacitor has an air gap of 5 mm. The capacitor is charged by a battery, maintaining a constant voltage. When a mica sheet of 2 mm thickness is introduced between the plates, it affects the capacitance, resulting in a 25% increase in charge.
The capacitance of a parallel plate capacitor without any dielectric is given by:
\(C_0 = \frac{\varepsilon_0 A}{d}\)
where:
When a dielectric material is partially inserted, the new capacitance can be described by considering the capacitor as two capacitors in series:
The new capacitance \(C_{new}\) is calculated using:
\(\frac{1}{C_{new}} = \frac{d_1}{\varepsilon_0 A} + \frac{d_2}{\varepsilon A \kappa}\)
where:
Using the relationship that the charge \(Q\) is proportional to capacitance \(Q = CV\), and knowing \(C_{new} = 1.25C_0\):
\(1.25C_0 = \frac{\varepsilon_0 A}{3} + \frac{\varepsilon A \kappa}{2}\)
Simplifying and solving for \(\kappa\):
\(1.25 = \frac{3\kappa + 2}{5}\)
By solving:
\(6.25 = 3\kappa + 2\)
\(3\kappa = 4.25\)
\(\kappa \approx 1.42\)
Given options, the closest and correct dielectric constant of mica is 2.
A point charge \(q = 1\,\mu\text{C}\) is located at a distance \(2\,\text{cm}\) from one end of a thin insulating wire of length \(10\,\text{cm}\) having a charge \(Q = 24\,\mu\text{C}\), distributed uniformly along its length, as shown in the figure. Force between \(q\) and wire is ________ N. 