To analyze the problem, let's break it down step-by-step:
\(F = \frac{k \cdot |q_1 \cdot q_2|}{r^2} = \frac{k \cdot |q \cdot (-2q)|}{r^2} = \frac{2kq^2}{r^2}\)
\(F' = \frac{k \cdot |\left(\frac{-q}{2}\right) \cdot \left(\frac{-q}{2}\right)|}{\left(\frac{r}{2}\right)^2}\)
Solving for \(F'\) gives:
\(F' = \frac{k \cdot \left(\frac{q^2}{4}\right)}{\frac{r^2}{4}} = \frac{k \cdot q^2}{r^2}\)
Hence, the force becomes half the magnitude of the initial force \(F\), and since the charges are both negative, they repel each other.
The correct answer is: They will repel with a force \(\frac{F}{2}\).
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. 