Step 1: Understanding the Concept:
The container is insulated, so no heat leaves. When it stops suddenly, the bulk kinetic energy of the gas turns into random thermal energy of molecules.
Step 2: Write the energy balance:
Let the mass of the gas be \(M\) and its molar mass be \(m\), so the number of moles is \(n=\dfrac Mm\). Kinetic energy lost \(=\dfrac12MV^2\).
Step 3: Internal energy gained:
For a monatomic gas, \(\Delta U=n\cdot\dfrac32R\,\Delta T=\dfrac Mm\cdot\dfrac32R\Delta T\).
Step 4: Solve:
\(\dfrac12MV^2=\dfrac{3MR}{2m}\Delta T\), so \(\Delta T=\dfrac{mV^2}{3R}\). Option C.
Step 5: Why the other options are wrong.
Options A and B ignore the \(\dfrac32R\) per mole for a monatomic gas (they use \(C_v=R\) or \(\dfrac R2\) instead). Option D uses \(\dfrac52R\), the value for a diatomic gas.
Final Answer:
The temperature rise is m V^2 / (3R).
\[ \boxed{\text{(C) }\dfrac{mV^2}{3R}} \]