Supersonic Speeds, Shock Waves — Question 8

Section 17-9 · Physics pages 2806–2807

Question 8 A finite-strength front need not make the Mach angle A straight front is attached to a source moving at v = 800 m/s through a still medium with small-disturbance speed c = 320 m/s. Its front angle to the backward flight axis is β. The front propagates normally into undisturbed material at speed D = 400 m/s; geometry gives v sin β = D. µ β v Weak Mach generator and steeper finite-strength front are distinguished. (a) Find the small-disturbance Mach angle and the actual front angle under the supplied model. (b) Explain why substituting 1/M for sin β would be wrong here. What condition recovers the Mach-angle result?
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Question 8 - Solution A finite-strength front need not make the Mach angle µ β v (a) Method and calculation The source Mach number is M = v/c = 2.5, giving µ = sin−1(c/v) = sin−1(0.4) = 23.578◦. The actual normal front speed instead gives β = sin−1(D/v) = sin−1(0.5) = 30◦. (b) Interpretation and further calculation The angle relation involves the speed at which the front advances normal to itself. Here D > c, so β > µ. Replacing D by c would assume the front is a weak acoustic disturbance. The limit D →c recovers β →µ; determining D from front strength would require additional material and conservation relations. Physical check The given model requires D ≤v for a real attached-front angle. It does not equate small-signal sound speed with finite-strength front speed.

Question 8

A finite-strength front need not make the Mach angle

A straight front is attached to a source moving at v=800m/sv=800\,\mathrm{m/s} through a still medium with small-disturbance speed c=320m/sc=320\,\mathrm{m/s}. Its front angle to the backward flight axis is β\beta. The front propagates normally into undisturbed material at speed D=400m/sD=400\,\mathrm{m/s}; geometry gives vsin⁡β=Dv\sin\beta=D.

Diagram shown in the original SVG worksheet.

  1. Find the small-disturbance Mach angle and the actual front angle under the supplied model.

  2. Explain why substituting 1/M1/M for sin⁡β\sin\beta would be wrong here. What condition recovers the Mach-angle result?

Question 8 - Solution

A finite-strength front need not make the Mach angle

Diagram shown in the original SVG worksheet.

(a) Method and calculation

The source Mach number is M=v/c=2.5M=v/c=2.5, givingμ=sin⁡−1(c/v)=sin⁡−1(0.4)=23.578∘.\mu=\sin^{-1}(c/v)=\sin^{-1}(0.4)=23.578^\circ.The actual normal front speed instead givesβ=sin⁡−1(D/v)=sin⁡−1(0.5)=30∘.\beta=\sin^{-1}(D/v)=\sin^{-1}(0.5)=30^\circ.

(b) Interpretation and further calculation

The angle relation involves the speed at which the front advances normal to itself. Here D>cD>c, so β>μ\beta>\mu. Replacing DD by cc would assume the front is a weak acoustic disturbance. The limit D→cD\to c recovers β→μ\beta\to\mu; determining DD from front strength would require additional material and conservation relations.

Physical check

The given model requires D≤vD\le v for a real attached-front angle. It does not equate small-signal sound speed with finite-strength front speed.