The electric field generated by a long straight wire is represented by the equation: 
\[ E = \frac{\lambda}{2\pi\epsilon_0 r} \] For two wires, the fields are: \[ E_1 = \frac{\lambda_1}{2\pi\epsilon_0 r_1}, \quad E_2 = \frac{\lambda_2}{2\pi\epsilon_0 r_2} \] With the given values substituted: \[ E_1 = \frac{10 \times 10^{-6}}{2\pi\epsilon_0 (10 \times 10^{-2})} (-\hat{j}) \] \[ E_2 = \frac{20 \times 10^{-6}}{2\pi\epsilon_0 (20 \times 10^{-2})} (-\hat{j}) \] The resultant electric field is calculated as: \[ E_{\text{net}} = \frac{10 \times 10^{-6}}{2\pi\epsilon_0} \left(\frac{1}{0.1} + \frac{2}{0.2} \right) (-\hat{j}) \] \[ E_{\text{net}} = 3.6 \times 10^6 (-\hat{j}) \text{ N/C} \] The force experienced by the electron is: \[ F_{\text{net}} = qE_{\text{net}} \] \[ F_{\text{net}} = (-1.6 \times 10^{-19}) \times (3.6 \times 10^6) \text{ N} \] \[ F_{\text{net}} = 5.76 \times 10^{-13} \text{ N } (\hat{j}) \]
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. 