\(3.536\times10^5 \)Pa
\(3.536\times10^6\) Pa
\(1.25\times10^6\) Pa
\(1.25\times10^5 \)Pa
To solve this problem, we need to apply the concepts of isothermal and adiabatic processes for an ideal gas.
Initially, we have a gas with volume \( V \), temperature \( 27^\circ C \) (or 300 K), and pressure \( 2 \times 10^7 \, \text{Nm}^{-2} \).
Step 1: Isothermal ExpansionDuring an isothermal process, the temperature remains constant. According to Boyle's Law for an isothermal process:
P_1 V_1 = P_2 V_2
Initially, V_1 = V and P_1 = 2 \times 10^7 \, \text{Nm}^{-2}. The volume, V_2, after doubling is 2V.
We have:
2 \times 10^7 \times V = P_2 \times 2V
Solving for P_2:
P_2 = \frac{2 \times 10^7}{2} = 1 \times 10^7 \, \text{Nm}^{-2}
Step 2: Adiabatic ExpansionIn an adiabatic process, no heat is exchanged. The equation for an adiabatic process is given by:
P_2 V_2^{\gamma} = P_3 V_3^{\gamma}
We have V_3 = 2V_2 = 4V and \gamma = 1.5.
Substituting the known values:
1 \times 10^7 \times (2V)^{1.5} = P_3 \times (4V)^{1.5}
Simplifying:
(2)^{1.5} = 2^{1.5} = \sqrt{8} = 2\sqrt{2}
P_3 = \frac{1 \times 10^7 \times 2^{1.5}}{4^{1.5}}
(4)^{1.5} = \sqrt{64} = 8
Thus:
P_3 = \frac{1 \times 10^7 \times 2\sqrt{2}}{8}
Calculating further:
P_3 = \frac{1 \times 10^7 \times 2\sqrt{2}}{8} = 3.536 \times 10^6 \, \text{Pa}
Thus, the final pressure of the gas is \(3.536 \times 10^6 \, \text{Pa}\), which is option B.