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The exit area of the nozzle in cm2 is

  • A.90.1
  • B.56.3
  • C.4.4
  • D.12.9

Answer: D

The exit area is about 12.9 cm2.

Take R = 287 J/kg.K for air. The mass flow rate at inlet is:

\[ \begin{aligned} \rho_{1} &= \frac{300\,000}{287 \times 500} = 2.091\ \text{kg/m}^{3} \\ \dot{m} &= 2.091 \times 0.008 \times 10 = 0.1673\ \text{kg/s} \end{aligned} \]

At exit, with T2 = 484 K from the previous question:

\[ \begin{aligned} \rho_{2} &= \frac{100\,000}{287 \times 484} = 0.720\ \text{kg/m}^{3} \\ A_{2} &= \frac{0.1673}{0.720 \times 180} = 12.9\ \text{cm}^{2} \end{aligned} \]

4.4 cm2 is what results from ignoring the density change (80 × 10/180). 90.1 and 56.3 cm2 would make the exit larger than or close to the inlet, which an accelerating subsonic nozzle does not do.

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