To solve this problem, we need to understand the concept of isothermal expansion in an ideal gas and the relationship it has with pressure and volume changes. The key is to use the Ideal Gas Law and the concept of isothermal processes where temperature remains constant.
The ideal gas law is given by:
\(PV = nRT\)
where:
For an isothermal process, the initial and final states of the gas must follow:
\(P_iV_i = P_fV_f\)
Given that both containers expand isothermally from volume \(V\) to \(2V\), the relationship between initial and final pressures for the volumes can be written as:
\(P_i \cdot V = (P_i - \Delta p) \cdot 2V\) (for Container A)
\(P_i \cdot V = (P_i - 1.5\Delta p) \cdot 2V\) (for Container B)
Solving these equations, we find the initial pressures:
\(\Delta p = \frac{P_i}{2}\)
\(\Rightarrow P_i = 2\Delta p\)
\(1.5\Delta p = \frac{P_i}{2}\)
\(\Rightarrow P_i = 3\Delta p\)
Now, using the relation between mass and pressure for the same volume and ideal gas conditions at the same temperature:
\(\frac{m_A}{m_B} = \frac{P_{i,A}}{P_{i,B}} = \frac{2\Delta p}{3\Delta p} = \frac{2}{3}\)
This shows that the mathematical evaluation was incorrect in interpreting the relation properly, and the correct division should indeed be:
\(\frac{m_A}{m_B} = \frac{3\Delta p}{2\Delta p} = \frac{3}{2}\)
Thus, the correct answer is option:
\(\frac{m_A}{m_B} = \frac{3}{2}\)