The problem is addressed using Coulomb's Law, which quantifies the force \( F \) between two point charges \( q_1 \) and \( q_2 \) at a separation \( r \) as: \( F = k \cdot \frac{q_1 \cdot q_2}{r^2} \), where \( k \) is Coulomb's constant. Initially, the force is: \( F = k \cdot \frac{q_1 \cdot q_2}{r^2} \). Subsequently, the distance is doubled to \( 2r \), and both charges are halved to \( \frac{q_1}{2} \) and \( \frac{q_2}{2} \). The resulting force, \( F' \), is calculated as: \( F' = k \cdot \frac{\left( \frac{q_1}{2} \right) \cdot \left( \frac{q_2}{2} \right)}{(2r)^2} \), which simplifies to: \( F' = k \cdot \frac{\frac{q_1 \cdot q_2}{4}}{4r^2} \) and further to: \( F' = k \cdot \frac{q_1 \cdot q_2}{16r^2} \). Comparing the new force \( F' \) to the original force \( F \), we find: \( F' = \frac{1}{16} \cdot k \cdot \frac{q_1 \cdot q_2}{r^2} \), which means \( F' = \frac{1}{16} \cdot F \). Consequently, the new force is \( \frac{F}{16} \).
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. 