22-Mec-A1 Applied Thermodynamics and Heat Transfer · May 2017
Question 3 of 8: Turbojet on a Static Test Bed — Nozzle Velocity and Thrust
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Reference texts: Çengel & Boles, Thermodynamics: An Engineering Approach (9th ed., McGraw-Hill) — closed- and open-system energy balances, filling of evacuated vessels, air-standard dual and gas-turbine (turbojet) cycles, and vapour-compression refrigeration; Çengel & Ghajar, Heat and Mass Transfer (6th ed.) and Incropera, DeWitt, Bergman & Lavine, Fundamentals of Heat and Mass Transfer (8th ed., Wiley) — radial composite-cylinder conduction with convection, external cross-flow over a cylinder, internal-flow temperature decay, radiation between concentric spheres with a shield, and the ε–NTU cross-flow heat-exchanger method. Ammonia and ideal-gas air properties are read from the tables appended to the examination paper; the turbojet uses cold-air-standard constant specific heats.
Paper format: National Examination 16-Mec-A1, May 2017, 3 hours, open book. Part A — Thermodynamics (Q1–4); Part B — Heat Transfer (Q5–8). Each answer carries equal value; a complete paper is any five (three questions from one part and two from the other). All eight questions are solved in full below.
Question 3: Turbojet on a Static Test Bed — Nozzle Velocity and Thrust (equal value)
Given. The cycle and ambient data above. Find. the nozzle exit velocity and the static thrust.
Figure 3 — Turbojet stations: 1 inlet, 2 compressor exit, 3 turbine inlet (max $T$), 4 turbine exit, 5 nozzle exit. The turbine produces exactly the compressor work; the remaining enthalpy drop accelerates the jet in the nozzle.
Approach. Work the compressor and turbine with their isentropic efficiencies (the turbine work equals the compressor work on a single spool), find the turbine-exit pressure, then expand isentropically in the nozzle, apply the nozzle efficiency to the kinetic energy, and get thrust from momentum ($\dot m V_5$ on a static bed).
Compressor (1→2). Ideal exit $T_{2s}=T_1r_p^{(\gamma-1)/\gamma}=253.15(8)^{0.2857}=458.6$ K; with $\eta_c$, $T_2=T_1+\dfrac{T_{2s}-T_1}{\eta_c}=486.6$ K, so $w_c=c_p(T_2-T_1)=234.6$ kJ/kg and $P_2=8P_1=810.6$ kPa.
Turbine (3→4), work = compressor work. $c_p(T_3-T_4)=w_c\Rightarrow T_4=T_3-\dfrac{w_c}{c_p}=1273.15-233.4=1039.7$ K. The isentropic drop is $T_3-T_{4s}=\dfrac{T_3-T_4}{\eta_t}$, giving $T_{4s}=1007.9$ K.
Nozzle isentropic expansion to ambient (4→5). $T_{5s}=T_4\left(\dfrac{P_1}{P_4}\right)^{(\gamma-1)/\gamma}=1039.7(0.2831)^{0.2857}=725.0$ K, so the ideal kinetic energy is $c_p(T_4-T_{5s})=316.3$ kJ/kg.
Actual jet velocity. Applying the nozzle efficiency, $\tfrac12V_5^{2}=\eta_n\,c_p(T_4-T_{5s})=0.90(316.3)=284.6$ kJ/kg, hence
$$V_5=\sqrt{2(284.6\times10^{3})}$$
$V_5\approx755$ m/s
Static thrust. On a stationary bed the inlet momentum is zero and the nozzle exhausts at ambient pressure, so $F=\dot m\,V_5=25(754.5)$.
$F\approx18.9$ kN