Step 1: Understanding the Concept
The emf of a curved conductor moving in a uniform field equals that of the straight line joining its ends.
Step 2: Calculation
PR is the horizontal diameter, length \(2r\). The velocity is downward, the field is into the page and the diameter is horizontal, all mutually perpendicular.
\(e=B\,v\,(2r)=2rBv\)
Step 3: Polarity
The force on positive charges, \(\vec{v}\times\vec{B}\) (down \(\times\) into the page), points towards R. So R is at the higher potential.
Final Answer:
The potential difference is \(2rBv\) with R at the higher potential.
\[ \boxed{\text{(C) }2rBv\text{ and terminal R is at higher potential}} \]