To solve this problem, we utilize the ideal gas law, which is stated as \(PV=nRT\). Here \(P\) is pressure, \(V\) is volume, \(n\) is the number of moles, \(R\) is the gas constant, and \(T\) is temperature in Kelvin. We assume the gas behaves ideally under given conditions.
First, convert temperatures from Celsius to Kelvin.
Initial temperature \(T_1\):
\(T_1=27^\circ\text{C}+273.15=300.15\,\text{K}\)
Final temperature \(T_2\):
\(T_2=77^\circ\text{C}+273.15=350.15\,\text{K}\)
The initial and final conditions are related by the equation:
\(\frac{P_1V_1}{T_1}=\frac{P_2V_2}{T_2}\)
Substitute the known values:
\(\frac{2\times60}{300.15}=\frac{P_2\times20}{350.15}\)
Solve for \(P_2\):
\(P_2=\frac{2\times60\times350.15}{300.15\times20}\)
After calculating,
\(P_2=7\), which is within the expected range (7,7).
Thus, the final pressure is \(7\) atmospheric pressure.
A real gas within a closed chamber at \( 27^\circ \text{C} \) undergoes the cyclic process as shown in the figure. The gas obeys the equation \( PV^3 = RT \) for the path A to B. The net work done in the complete cycle is (assuming \( R = 8 \, \text{J/molK} \)):
