
To solve this problem, we need to determine the potential difference developed across the semicircular conducting ring when it is moving in a magnetic field.
Given:
We will use the concept of motional EMF. When a conductor moves in a magnetic field, an electromotive force (EMF) is induced across its ends. The formula for EMF (\( \mathcal{E} \)) induced in a conductor of length \( L \) moving with velocity \( v \) perpendicular to a magnetic field \( B \) is given by:
\(\mathcal{E} = BvL\)
For a semicircular wire, the length of the wire from \( P \) to \( R \) through \( Q \) is \( \pi r \), but the effective length across which the EMF is induced is the straight line distance from \( P \) to \( R \), which is the diameter of the semicircle, i.e., \( 2r \).
Thus, the induced EMF (potential difference) is:
\(\mathcal{E} = Bv(2r) = 2rBv\)
Determining the polarity: As the ring falls, electrons in the segment PR will drift towards R due to the magnetic force, making R at a higher potential.
Therefore, the correct answer is: 2rBv and R is at higher potential.