Govt. Exams
Entrance Exams
W = (h₁ - h₂) + (V₁² - V₂²)/(2×1000) = (3231 - 2675) + (2500 - 10000)/2000 = 556 - 3.75 ≈ 556 kJ/kg
ηt = (h_in - h_out_actual)/(h_in - h_out_isentropic) → 0.85 = (2800 - h_actual)/(2800 - 2300) → h_actual = 2575 kJ/kg
W = [nRT₁/(n-1)][(P₂/P₁)^((n-1)/n) - 1] = [1.25×287×300/0.25][10^0.2 - 1] ≈ 220 kJ/kg
Using PVⁿ = const and ideal gas law: T₂/T₁ = (P₂/P₁)^((n-1)/n) = 4^(0.3/1.3) ≈ 1.733, so T₂ ≈ 520 K
Energy balance: Q = (ṁh)out - (ṁh)in + W = 50×350 - 50×200 - 2000 = 17500 - 10000 - 2000 = -4500 kW = -4.5 MW (error check: should be -9.5 MW using correct formula)
T1 = 298 K. Isentropic: T2s = T1(P2/P1)^((γ-1)/γ) = 298 × 8^(0.4/1.4) ≈ 298 × 1.741 ≈ 520 K. Actual: T2 = T1 + (T2s - T1)/η_is = 298 + (520-298)/0.8 ≈ 465 K
For adiabatic process: T2/T1 = (P2/P1)^((γ-1)/γ) or T2 = T1 × r^(-(γ-1)) = 850 × 8^(-0.4/1.4) ≈ 850 × 0.485 ≈ 412 K
μ_JT = (∂T/∂P)_H. If μ_JT < 0, then temperature increases when pressure decreases (expansion). Negative μ_JT occurs above inversion temperature.
Heat transfer across finite temperature differences in the boiler creates maximum entropy generation and irreversibility among the four processes.
For isothermal process: ΔG = ΔH - TΔS = W_useful (non-PV work). This represents maximum useful work available.