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Expansion Waves Questions and Answers

Answer: A

A sharp edge asks only a small deflection, which an attached weak oblique shock can supply, so the wave drag is small. A rounded edge would force a detached bow shock with a strong nearly normal portion ahead of it and a heavy drag penalty at supersonic speed.

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Answer: B

In supersonic flow the pressures on forward-facing and rearward-facing surfaces no longer balance, and the residue is a drag that exists even with no viscosity and no finite span. It is quite distinct from induced drag, which needs a finite wing, and from friction drag, which needs viscosity.

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Answer: C

The two waves interact: the expansion reduces the pressure ratio the shock has to sustain and so weakens it, while the shock refracts the characteristics of the fan. This is why the trailing-edge shocks of a supersonic aerofoil are weakened by the expansion coming off the surface ahead of them.

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24.

A convex corner in a supersonic stream can turn the flow through, at most,

Answer: D

Expansion is limited by the pressure falling to zero, at which point the gas has reached its maximum possible speed and cannot expand further. Turning beyond that leaves a vacuum region between the flow and the surface, so the flow simply separates from the corner.

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Answer: A

The corner is treated as sharp and the fan as centred, so no length scale enters and the solution is self-similar. Everything downstream follows from the upstream Mach number and the angle turned through, which is what makes the Prandtl-Meyer function such an economical piece of bookkeeping.

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26.

For air, the Prandtl-Meyer function evaluated at \( M = 2 \) is nearest to

Answer: B

The standard value is \( \nu(2) = 26.38 \) degrees. It says that a sonic stream must be turned through just over twenty-six degrees to reach Mach 2. The other options are the function evaluated at Mach 1.5 and Mach 3, and the Mach angle at Mach 2.

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27.

A stream at \( M_1 = 1.5 \), for which \( \nu = 11.90 \) degrees, is turned through \( 14.48 \) degrees round a convex corner. The downstream Mach number is

Answer: C

Turning angles add in the Prandtl-Meyer function, so \( \nu_2 = 11.90 + 14.48 = 26.38 \) degrees. Reading that value back gives \( M_2 = 2.0 \). This additivity is the whole reason the function is tabulated: no iteration is required.

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28.

Air already at \( M = 2 \), where \( \nu = 26.38 \) degrees, negotiates a convex corner of \( 23.38 \) degrees. What Mach number does it reach?

Answer: D

Adding the turn gives \( \nu_2 = 26.38 + 23.38 = 49.76 \) degrees, which corresponds to \( M = 3.0 \). Note how much turning the second unit of Mach number costs compared with the first: the function flattens as the Mach number rises.

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29.

The maximum angle through which a sonic stream of air can theoretically be turned by expansion is nearest to

Answer: A

The limit is \( \nu(\infty) = 90^\circ (\sqrt{(\gamma+1)/(\gamma-1)} - 1) \). With \( \gamma = 1.4 \) the square root is \( \sqrt{6} = 2.449 \), so the value is \( 90 \times 1.449 = 130.45 \) degrees. At that point the pressure has fallen to zero and no further expansion is possible.

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30.

The leading Mach line of an expansion fan in a stream at \( M_1 = 2 \) lies at what angle to the oncoming flow?

Answer: B

The leading characteristic is a Mach wave in the undisturbed flow, so it lies at the upstream Mach angle \( \arcsin(1/2) = 30 \) degrees. The distractor 19.5 degrees is the Mach angle at Mach 3, which would bound the fan if the flow were expanded to that speed.

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