When a parallel plate capacitor is energized by an AC source, an examination of current and voltage behavior at the plates is necessary to determine the applicability of Kirchhoff's first rule (junction rule) at these locations.
Kirchoff's first rule, also known as the junction rule, posits that at any junction, the aggregate of currents flowing in must equal the aggregate of currents flowing out. This principle is mathematically represented as:
\[ \sum I_{\text{in}} = \sum I_{\text{out}} \]
This tenet is founded upon the principle of charge conservation, asserting that charge cannot be generated or extinguished at a junction.
Upon connection to an AC source, the voltage across the capacitor plates undergoes sinusoidal variation. As AC current circulates, it induces charge accumulation on the plates, leading to oscillatory charge behavior synchronous with the alternating voltage.
In this configuration:
Initially, it may appear that Kirchhoff's first rule is inapplicable to capacitor plates due to the absence of direct current flow through the dielectric. However, the junction rule remains valid when considering the displacement current within the capacitor plates, which is intrinsically linked to the changing electric field between them. The definition of displacement current is as follows:
Affirmative, Kirchhoff's first rule (junction rule) is applicable to each plate of the capacitor within an AC circuit, provided that displacement current is incorporated into the analysis. This displacement current is the mechanism for the plates' charging and discharging, thereby ensuring that the currents entering and leaving the capacitor plates adhere to the junction rule, consistent with its behavior at any other circuit junction.
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. 