Step 1: Think about what changes:
Temperature is fixed, so the internal energy of an ideal gas is fixed: $\Delta U = 0$.
Step 2: Match each option:
Writing $\Delta U = Q + W$ with $\Delta U = 0$ gives $W = -Q$, exactly option (A).
The other expressions describe other conditions: B has no heat term (adiabatic), C has $W = 0$ (constant volume), D uses constant external pressure.
Final Answer:
The isothermal form of the first law is $W = -Q$, option (A).
\[ \boxed{W = -Q} \]