Process I is adiabatic reversible
Process II is a reversible isothermal process
Process I – (Adiabatic Reversible)
\(\frac{\Delta U}{R} = 450 - 2250\)
∆U = -1800 R
WI = ∆U = -1800R
Process II – (Reversible Isothermal Process)
T1 = 900 K
Calculation of T2 after the reversible adiabatic process
–1800R = nCv(T2 – T1)
\(-1800R \times \frac{1 \times 5}{2} R(T_2 - 900)\)
T2 = 180 K
WII = –nRT2 In = W
\(-1 \times R \times 180 \ln \frac{v_3}{v_2} -1800R\)
\(\ln \frac{v_3}{v_{2}}=10\)
List-I | List-II | ||
(A) | Isothermal process | (I) | No heat exchange |
(B) | Isochoric process | (II) | Carried out at constant temperature |
(C) | Isobaric process | (III) | Carried out at constant volume |
(D) | Adiabatic process | (IV) | Carried out at constant pressure |