
To solve this problem, we need to calculate the magnetic force per unit length between two parallel current-carrying conductors, specifically wires \(PQ\) and \(RS\) of the rectangular loop.
The formula for the magnetic force per unit length \(f\) between two parallel wires carrying currents \(I_1\) and \(I_2\) and separated by distance \(d\) is given by:
\(f = \frac{\mu_0 I_1 I_2}{2\pi d}\)
In this scenario, initially, both wires \(PQ\) and \(RS\) carry the same current \(I\). When the current in the circuit changes from \(I\) to \(2I\), we need to find the ratio of the forces per unit length in these two conditions.
Now, calculate the ratio:
\(\frac{f_{PQ}^I}{f_{PQ}^{2I}} = \frac{\frac{\mu_0 I^2}{2\pi d}}{\frac{\mu_0 \cdot 4I^2}{2\pi d}} = \frac{I^2}{4I^2} = \frac{1}{4}\)
Thus, the ratio of magnetic forces per unit length when the current is \(I\) and \(2I\) is \(1:4\).
Therefore, the correct answer is: \(1:4\)
A parallel plate capacitor of area \( A = 16 \, \text{cm}^2 \) and separation between the plates \( 10 \, \text{cm} \), is charged by a DC current. Consider a hypothetical plane surface of area \( A_0 = 3.2 \, \text{cm}^2 \) inside the capacitor and parallel to the plates. At an instant, the current through the circuit is 6A. At the same instant the displacement current through \( A_0 \) is _____ mA.