Q2: Helium, at To = 400 K, enters a nozzle isentropically. At section 1, where A1 = 0.1 m2, a pitot-static arrangement (see Fig. Q2) measures stagnation pressure of 150 kPa and static pressure of 123 kPa. Estimate (a) M1; (b) Tị; (c) mass flow; and (d) A*. Take y = 1.66 and R = 2077 J/(kg-K). Air at 100 K Mercury Ans. (a) 0.5; (b) 370 K; (c) 9.03 kg/s; and (d) 0.0756 m².

Elements Of Electromagnetics
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Q2: Helium, at T. = 400 K, enters a nozzle isentropically. At section 1, where Aj = 0.1 m, a
pitot-static arrangement (see Fig. Q2) measures stagnation pressure of 150 kPa and static
pressure of 123 kPa. Estimate (a) M1; (b) T;; (c) mass flow; and (d) A*. Take y = 1.66 and
R = 2077 J/(kg K).
Air at 100 K
Mercury
Ans. (a) 0.5; (b) 370 K; (c) 9.03 kg/s; and (d) 0.0756 m2.
Transcribed Image Text:Q2: Helium, at T. = 400 K, enters a nozzle isentropically. At section 1, where Aj = 0.1 m, a pitot-static arrangement (see Fig. Q2) measures stagnation pressure of 150 kPa and static pressure of 123 kPa. Estimate (a) M1; (b) T;; (c) mass flow; and (d) A*. Take y = 1.66 and R = 2077 J/(kg K). Air at 100 K Mercury Ans. (a) 0.5; (b) 370 K; (c) 9.03 kg/s; and (d) 0.0756 m2.
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