Step 1: Why work is needed.
Sliding the wire $CD$ changes the area of the loop, which changes the flux and drives a current. The external agent must supply power to keep it moving steadily.
Step 2: Energy shortcut.
When the rod moves at constant speed, all the work done per second by the agent ends up dissipated as heat in the resistor. So work done per second equals the power lost in $R$.
Step 3: Motional emf.
The rod of length $l$ moving at speed $v$ across field $B$ sets up \[ \varepsilon=Blv. \]
Step 4: Power dissipated in the resistor.
Using $P=\dfrac{\varepsilon^2}{R}$, \[ P=\frac{(Blv)^2}{R}. \]
Step 5: Simplify.
\[ P=\frac{B^2 l^2 v^2}{R}. \]
Step 6: Read off the answer.
Work done per second to slide the wire equals this power.
\[ \boxed{\dfrac{B^2 l^2 v^2}{R}} \]