The problem at hand involves the calculation of the potential difference generated across the ends of a metallic rod rotating in a magnetic field.
Firstly, let's understand the concept involved:
When a conductive rod rotates in a magnetic field, an electromotive force (emf) is induced across its ends due to electromagnetic induction. This can be calculated using the formula:
EMF = B \cdot \omega \cdot l^2 / 8
where:
Let's substitute the values given in the problem:
Therefore, the potential difference (emf) can be calculated as:
EMF = \frac{0.5 \cdot 2 \cdot 4^2}{8}
EMF = \frac{0.5 \cdot 2 \cdot 16}{8}
EMF = 2 \, \text{V}
However, on close inspection, it appears there is a misunderstanding. As we are calculating the potential difference across the ends of the rod when it is rotating about its perpendicular bisector:
Since the rod rotates about its perpendicular bisector, the effective length l_{\text{eff}} for the potential difference calculation is zero (due to symmetry about the axis of rotation), hence:
EMF = 0
This implies there is no net induced emf across the entire rod, which reaffirms that the potential difference developed across the ends of the rod is indeed 0 \, \text{V}.
Thus, the correct answer is:

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: