Step 1: Understanding the Concept:
The figure shows a rectangular circuit with a resistor on the left and a rod of length \(L\) on the right moving with speed \(V\) in a field \(B\) pointing into the page. The flux through the loop grows, so an emf appears.
Step 2: Emf and current:
\[ \varepsilon = BLV, \qquad I = \frac{\varepsilon}{R} = \frac{BLV}{R} \]
Step 3: Magnetic force on the rod:
The current in the rod feels a force \(F = BIL\), directed opposite to the motion (Lenz's law).
\[ F = B\cdot\frac{BLV}{R}\cdot L = \frac{B^2L^2V}{R} \]
Step 4: Result:
To keep a constant speed the applied force must equal this magnetic force, option (B). Option (A) \(BVL/R\) is not a force, since it equals the current in amperes. Options (C) and (D) have an extra factor of \(V\), which does not fit a force.
Final Answer:
The applied force must match B I L = B^2 L^2 V / R.
\[ \boxed{\text{(B) }\dfrac{B^2L^2V}{R}} \]