Step 1: Understanding the Concept
For an ideal gas, \(pV=\frac{m}{M}RT\), so the initial pressure \(p=\frac{mRT}{MV}\) is proportional to the mass \(m\).
Step 2: Isothermal expansion
For expansion from \(V\) to \(2V\) at constant \(T\), \(p_{f}=\frac{p}{2}\). So \(\Delta p=\frac{p}{2}=\frac{mRT}{2MV}\).
Step 3: Calculation
\(\Delta p\propto m\). For A, \(\Delta p=\frac{m_{A}RT}{2MV}\) and for B, \(3\Delta p=\frac{m_{B}RT}{2MV}\).
Step 4: Ratio
Dividing, \(3=\frac{m_{B}}{m_{A}}\), that is \(3m_{A}=m_{B}\), which is option (C).
Final Answer:
The masses satisfy \(3m_{A}=m_{B}\).
\[ \boxed{\text{(C) }3m_{A}=m_{B}} \]