To solve the problem, we need to understand the thermodynamics of a sudden expansion. The process is likely adiabatic since it happens suddenly, meaning no heat is exchanged with the surroundings.
The adiabatic process is governed by:
\(P_1 V_1^\gamma = P_2 V_2^\gamma\)
Given:
The adiabatic index \(\gamma\) is given by:
\(\gamma = \frac{C_p}{C_v}\)
Using the relation \(C_p = C_v + R\), we have:
\(\gamma = \frac{C_v + R}{C_v} = \frac{2R + R}{2R} = \frac{3}{2}\)
Now apply the adiabatic condition:
\(P_1 V_1^{\frac{3}{2}} = P_2 (3V_1)^{\frac{3}{2}}\)
Simplifying, we get:
\(P_1 = P_2 \cdot 3^{\frac{3}{2}}\)
Hence, the ratio of initial to final pressures is:
\(\frac{P_1}{P_2} = 3^{\frac{3}{2}} = 3 \times \sqrt{3} \approx 5.2\)
Considering significant options, the closest answer is 5.
Thus, the ratio of initial to final pressures is nearly equal to 5.