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Nozzles and Thrust Generation Questions and Answers

21.

An engine passes \( 80 \ \mathrm{kg/s} \) with an exit velocity of \( 500 \ \mathrm{m/s} \) while flying at \( 200 \ \mathrm{m/s} \). The net thrust, ignoring pressure terms and fuel flow, is

Answer: A

Net thrust is the mass flow times the velocity increment, \( 80 \times (500-200) = 24\,000 \) newtons. The gross thrust would be 40 kilonewtons, and the 16 kilonewton difference is exactly the ram drag of the incoming air.

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22.

For the same engine at rest on the ground, the thrust is

Answer: B

With no flight speed there is no ram drag, so gross and net thrust are equal at \( 80 \times 500 = 40\,000 \) newtons. That is precisely why a static thrust figure overstates what the engine delivers once the aircraft is moving.

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23.

A nozzle of exit area \( 0.5 \ \mathrm{m^2} \) has an exit pressure of \( 120 \ \mathrm{kPa} \) against an ambient of \( 101 \ \mathrm{kPa} \). The pressure thrust is

Answer: C

Correct answer: 9.5 kN

The pressure thrust is the excess of exit over ambient pressure acting on the exit area:

\[ F_p = (p_e - p_a)A_e = (120 - 101)\times10^3 \times 0.5 = 9500 \text{ N} = 9.5 \text{ kN} \]

This term appears when the nozzle is choked and the flow leaves under-expanded, the remaining expansion taking place outside in the free jet. The 19 kN answer omits the area, and 60 kN uses the exit pressure rather than the difference.

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24.

The critical pressure ratio is \( ((\gamma+1)/2)^{\gamma/(\gamma-1)} \). For \( \gamma = 1.33 \) it is approximately

Answer: D

Correct answer: 1.85

Substituting \( \gamma = 1.33 \), which is representative of hot combustion products,

\[ \left(\frac{\gamma+1}{2}\right)^{\frac{\gamma}{\gamma-1}} = (1.165)^{4.03} \approx 1.85 \]

so the nozzle chokes once the total-to-ambient pressure ratio reaches about 1.85. For cold air, with \( \gamma = 1.4 \), the figure is 1.89. The reciprocal, 0.53, is the critical pressure ratio written the other way up, as static over total.

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25.

An engine has a nozzle pressure ratio of 3.2 against a critical ratio of 1.85. The nozzle is

Answer: A

The available ratio well exceeds critical, so a convergent nozzle chokes and the remaining expansion occurs outside it. Fitting a divergent section would convert that residual pressure into velocity and recover part of the loss.

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26.

Exhaust gas at 900 K expands isentropically to an exit velocity given by \( V = \sqrt{2 c_p \Delta T} \). With \( c_p = 1150 \) and a drop of 150 K, the velocity is approximately

Answer: B

Substituting gives \( \sqrt{2 \times 1150 \times 150} = \sqrt{345\,000} \approx 587 \) metres per second. Every kelvin of temperature drop that the nozzle fails to convert appears as lost exit velocity and therefore lost thrust.

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27.

A nozzle has a coefficient of velocity of 0.98. Its ideal exit velocity of \( 600 \ \mathrm{m/s} \) becomes

Answer: C

Correct answer: 588 m/s

The coefficient of velocity is the ratio of actual to ideal exit velocity:

\[ V_e = C_v V_{ideal} = 0.98 \times 600 = 588 \text{ m/s} \]

The two per cent shortfall represents friction and non-uniformity in the nozzle. A coefficient of velocity above unity is impossible, since the ideal is the isentropic case, so the answers above 600 m/s can be rejected without calculation.

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28.

An engine produces \( 60 \ \mathrm{kN} \) at sea level. At a density ratio of 0.35, assuming thrust scales with density, it produces approximately

Answer: D

Correct answer: 21 kN

With thrust proportional to density,

\[ F = 60 \times 0.35 = 21 \text{ kN} \]

Mass flow through a given engine is proportional to the density of the air it swallows, and thrust follows it directly, which is why an engine at 11 km produces roughly a third of its sea level thrust. This lapse is what sets the cruise altitude ceiling and why take-off thrust ratings are quoted at sea level.

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29.

A turbofan of \( 300 \ \mathrm{kg/s} \) total flow produces \( 60 \ \mathrm{kN} \). Its specific thrust is

Answer: A

Correct answer: 200 N per kg/s

Specific thrust is thrust divided by air mass flow:

\[ F_s = \frac{60\,000}{300} = 200 \text{ N per kg/s} \]

Two hundred is typical of a high bypass turbofan, which makes its thrust from a large mass of air given a small velocity increment. A turbojet works near 800, passing a quarter of the air at four times the increment, which is why it is so much smaller and so much less efficient at subsonic speed.

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30.

Jet noise power varies roughly with the eighth power of jet velocity. Halving the jet velocity reduces the noise power by a factor of about

Answer: B

Halving gives \( (1/2)^8 = 1/256 \), a reduction of about 24 decibels. That extraordinary sensitivity is why raising bypass ratio, which lowers jet velocity, transformed aircraft noise more than any acoustic treatment could.

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