Supersonic Speeds, Shock Waves — Question 1

Section 17-9 · Physics pages 2792–2793

Question 1 A Mach cone is an envelope of earlier sound fronts A compact source moves uniformly at v = 680 m/s through still air with small-disturbance sound speed c = 340 m/s. Assume steady motion extending sufficiently far into the past and the weak-disturbance cone construction. S µ v Cross-section of the cone tangent to an earlier spherical wavefront; the source moves right. (a) Derive the relation between Mach number M = v/c and cone half-angle µ. (b) Find M and µ. Explain why the relevant angle uses a sine, not a tangent.
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Question 1 - Solution A Mach cone is an envelope of earlier sound fronts S µ v (a) Method and calculation A disturbance emitted a time τ earlier occupies a sphere of radius cτ centered at the old source position. The current source is vτ from that center. The cone is tangent to the sphere; the radius to the tangent point is perpendicular to the cone generator. The right triangle therefore gives sin µ = cτ vτ = c v = 1 M . (b) Interpretation and further calculation Numerically, M = 680/340 = 2 and µ = sin−1(1/2) = 30◦. The source-to-old-center segment is the hypotenuse, not a leg, in the tangency triangle. Using tan µ = c/v would instead predict 26.565◦and the wrong envelope. Physical check A real Mach angle requires M ≥1; a finite cone with 0 < µ < 90◦requires supersonic motion.

Question 1

A Mach cone is an envelope of earlier sound fronts

A compact source moves uniformly at v=680m/sv=680\,\mathrm{m/s} through still air with small-disturbance sound speed c=340m/sc=340\,\mathrm{m/s}. Assume steady motion extending sufficiently far into the past and the weak-disturbance cone construction.

Diagram shown in the original SVG worksheet.

  1. Derive the relation between Mach number M=v/cM=v/c and cone half-angle μ\mu.

  2. Find MM and μ\mu. Explain why the relevant angle uses a sine, not a tangent.

Question 1 - Solution

A Mach cone is an envelope of earlier sound fronts

Diagram shown in the original SVG worksheet.

(a) Method and calculation

A disturbance emitted a time τ\tau earlier occupies a sphere of radius cτc\tau centered at the old source position. The current source is vτv\tau from that center. The cone is tangent to the sphere; the radius to the tangent point is perpendicular to the cone generator. The right triangle therefore givessin⁡μ=cτvτ=cv=1M.\sin\mu=\frac{c\tau}{v\tau}=\frac c v=\frac1M.

(b) Interpretation and further calculation

Numerically, M=680/340=2M=680/340=2 and μ=sin⁡−1(1/2)=30∘\mu=\sin^{-1}(1/2)=30^\circ. The source-to-old-center segment is the hypotenuse, not a leg, in the tangency triangle. Using tan⁡μ=c/v\tan\mu=c/v would instead predict 26.565∘26.565^\circ and the wrong envelope.

Physical check

A real Mach angle requires M≥1M\ge1; a finite cone with 0<μ<90∘0<\mu<90^\circ requires supersonic motion.