Step 1: Recall how work is defined for a gas.
The work done by a gas as it changes volume is the integral of pressure over the volume change:
\[ W = \int_{V_1}^{V_2} P \, dV \]
Step 2: Apply the isovolumetric condition.
Isovolumetric means the volume stays fixed throughout the process, so \( V_1 = V_2 \). The limits of the integral become equal to each other.
Step 3: Evaluate the integral.
An integral taken from a point back to the same point is always zero, regardless of what the pressure is doing in between:
\[ W = \int_{V_1}^{V_1} P \, dV = 0 \]
This holds here even though the pressure itself drops to half its starting value, since it is the volume change, not the pressure change, that determines work.
Step 4: Final Answer.
\[ \boxed{W = 0\,J} \]