The mass is m = 0.05kg, μ = 44g/mol , the initial volume is,V1 = 0.03m3, the initial pressure is p1 = 1.025bar = 1.025⋅105Pa .
The final pressure is p2 = 6.15 bar = 6.15⋅105Pa.
(i) If pV1.4 = constant, then \(p_1 V^{1.4}_1 = p_2 V_2^{1.4} \Rightarrow V_2 = V_1(\frac {P_1}{P_2})= 8.3.10^{-3}m^3.\)
For such a polytropic process the work can be calculated as
\(A = \int pdV = v \frac {R}{1.4 -1}.T_1 (1 - \frac {T_2}{T_1}).\)
\(p_1 V_1 =\frac {m}{\mu}RT_1,T_1 = 325.6 K; \,\,p_2 V_2 = \frac {m}{\mu}RT_2, T_2 = 540.5 K.\)
Therefore, the work of gas will be \(A= v \frac {R}{1.4 - 1}.T_1 (1 - \frac {T _2}{T_1})= -5073J.\)
The heat that should be given to gas can be calculated as
\(q = \int T\,ds = v c_v \frac {1.4 - 1.3}{1.4 - 1} (T_2 - T _1) = 3R .v.\frac {1.4 - 1.3}{1.4 - 1}(540.5 - 325 .6) = 1522J.\)
(ii) In the isothermal process T1 = T2 = 325.6 K. For such process work can be calculated as \(A= \int p\,dV = vRT \,ln \frac {V_2}{V_1} =vRT \,ln \frac {p_1}{p_2} = -5509 J.\) The change of internal energy is 0, so the heat that should be given to the gas is -5509.J.
(iii) if the cylinder is thermally insulated the heat flow will be 0, so the process will be adiabatic.
Let us calculate the final temperature:
\(pV ^{1.3} = constant ,\,\, p_1 V^{1.3}_1 =p_2V ^{1.3} _2 \Rightarrow V_2 = V_1 (\frac {p_1}{p_2})^{1/1.3}= 7.56 .10^{-3}m^3.\)
\(p_2 V_2 = \frac {m}{\mu}RT_2, T_2 = 492 .4 K.\)
The work of the gas is equal to
\(A = -(U_2 - U_1)=c_vv(T_1 - T_2)=3Rv (T_1 - T _2) = -4725 J.\)
We may notice that the work of the gas is negative, so we should do work on gas.