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
\(-1 \times R \times 180 \ln \frac{v_3}{v_2} -1800R\)
\(\ln \frac{v_3}{v_{2}}=10\)
Match List-I with List-II.
Choose the correct answer from the options given below :
The ratio of the fundamental vibrational frequencies \( \left( \nu_{^{13}C^{16}O} / \nu_{^{12}C^{16}O} \right) \) of two diatomic molecules \( ^{13}C^{16}O \) and \( ^{12}C^{16}O \), considering their force constants to be the same, is ___________ (rounded off to two decimal places).}
A heat pump, operating in reversed Carnot cycle, maintains a steady air temperature of 300 K inside an auditorium. The heat pump receives heat from the ambient air. The ambient air temperature is 280 K. Heat loss from the auditorium is 15 kW. The power consumption of the heat pump is _________ kW (rounded off to 2 decimal places).