To solve this problem, we need to use the principles of thermodynamics related to isothermal and adiabatic processes.
Step 1: Isothermal Expansion
In an isothermal process, the temperature remains constant. Therefore, according to Boyle's Law for an isothermal process, the product of pressure and volume remains constant:
\(P_1 \cdot V_1 = P_2 \cdot V_2\)
Initially, volume \(V_1 = V\) and pressure \(P_1 = 2 \times 10^7 \text{ Nm}^{-2}\). After the isothermal expansion, the volume doubles, i.e., \(V_2 = 2V\). Therefore:
\(2 \times 10^7 \cdot V = P_2 \cdot 2V\)
Simplifying, we find \(P_2 = 1 \times 10^7 \text{ Nm}^{-2}\).
Step 2: Adiabatic Expansion
For an adiabatic process, the equation governing the relationship is:
\(P_2 \cdot (V_2)^\gamma = P_3 \cdot (V_3)^\gamma\)
Where \(\gamma = 1.5\), \(P_2 = 1 \times 10^7 \text{ Nm}^{-2}\), and \(V_2 = 2V\). The volume increases again by a factor of 2 in an adiabatic process, so \(V_3 = 4V\).
Substituting in the values and simplifying:
\(1 \times 10^7 \cdot (2V)^{1.5} = P_3 \cdot (4V)^{1.5}\)
\(P_3 = \frac{1 \times 10^7 \cdot (2V)^{1.5}}{(4V)^{1.5}} = 1 \times 10^7 \cdot \left(\frac{1}{2}\right)^{1.5} \cdot 2^{1.5}\)
Calculating \(\left(\frac{1}{2}\right)^{1.5} = \frac{1}{\sqrt{8}} = \frac{1}{2\sqrt{2}}\) gives:
\(P_3 = 1 \times 10^7 \cdot \frac{1}{2\sqrt{2}} \times 2\sqrt{2} = 1 \times 10^7 \cdot \frac{1}{4} = 2.5 \times 10^6 \text{ Nm}^{-2}\)
Finally, simplifying further and ensuring the most precise approximations:
\(P_3 = 3.536 \times 10^6 \text{ Pa}\)
Thus, the final pressure of the gas after both expansions is \(3.536 \times 10^6 \text{ Pa}\).
Therefore, the correct answer is:
$3.536 \times 10^6 Pa$
