Sound Waves — Question 7

Section 17-1 · Physics pages 2644–2645

Question 7 Reciprocal acoustic timing separates wind from sound speed Two stationary stations are separated by L = 100 m along uniform air flow. Sound takes t+ = 0.250 s downstream and t−= 0.3125 s upstream. Let c be sound speed relative to air and w < c the flow speed. A B w Propagation path; the stated distances determine travel time. (a) Infer c and w from these measurements. (b) Find the round-trip time and show why using it alone with still-air ranging overestimates the actual distance when c is known.
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Question 7 - Solution Reciprocal acoustic timing separates wind from sound speed A B w (a) Method and calculation The ground speeds are c + w and c −w, so c = L 2 ( 1 t+ + 1 t− ) = 360 m/s, w = L 2 ( 1 t+ −1 t− ) = 40 m/s. (b) Interpretation and further calculation The round-trip time is trt = L c + w + L c −w = 2Lc c2 −w2 = 0.5625 s. A still-air interpretation gives Lapp = ctrt/2 = 101.25 m. More generally Lapp/L = 1/[1 −(w/c)2] > 1: the upstream delay exceeds the downstream saving. Physical check The round-trip correction starts at order (w/c)2; a one-way timing difference is first order in flow.

Question 7

Reciprocal acoustic timing separates wind from sound speed

Two stationary stations are separated by L=100mL=100\,\mathrm m along uniform air flow. Sound takes t+=0.250st_+=0.250\,\mathrm s downstream and t−=0.3125st_-=0.3125\,\mathrm s upstream. Let cc be sound speed relative to air and w<cw<c the flow speed.

Diagram shown in the original SVG worksheet.

  1. Infer cc and ww from these measurements.

  2. Find the round-trip time and show why using it alone with still-air ranging overestimates the actual distance when cc is known.

Question 7 - Solution

Reciprocal acoustic timing separates wind from sound speed

Diagram shown in the original SVG worksheet.

(a) Method and calculation

The ground speeds are c+wc+w and c−wc-w, soc=L2(1t++1t−)=360m/s,c=\frac L2\left(\frac1{t_+}+\frac1{t_-}\right)=360\,\mathrm{m/s},w=L2(1t+−1t−)=40m/s.w=\frac L2\left(\frac1{t_+}-\frac1{t_-}\right)=40\,\mathrm{m/s}.

(b) Interpretation and further calculation

The round-trip time istrt=Lc+w+Lc−w=2Lcc2−w2=0.5625s.t_{\mathrm{rt}}=\frac L{c+w}+\frac L{c-w}=\frac{2Lc}{c^2-w^2}=0.5625\,\mathrm s.A still-air interpretation gives Lapp=ctrt/2=101.25mL_{\mathrm{app}}=ct_{\mathrm{rt}}/2=101.25\,\mathrm m. More generally Lapp/L=1/[1−(w/c)2]>1L_{\mathrm{app}}/L=1/[1-(w/c)^2]>1: the upstream delay exceeds the downstream saving.

Physical check

The round-trip correction starts at order (w/c)2(w/c)^2; a one-way timing difference is first order in flow.