Intensity and Sound Level — Question 4

Section 17-5 · Physics pages 2718–2719

Question 4 A level drop can determine an unknown geometric range An isotropic point source is at height h above a flat reference plane. One receiver is directly below it; another is 30.0 m horizontally away. The farther receiver measures 6.0206 dB less intensity level. Neglect reflections and absorption. S h 30 m Geometric range comparison; ground reflection is excluded. (a) Infer h using spherical spreading. (b) If the source power doubles, determine whether the inferred height or the level difference changes.
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Question 4 - Solution A level drop can determine an unknown geometric range S h 30 m (a) Method and calculation For equal source power, I ∝1/r2. The level difference gives Inear Ifar = 106.0206/10 = 4.000, rfar rnear = 2. √ h2 + 302 = 2h ⇒3h2 = 900 ⇒h = 17.32 m. (b) Interpretation and further calculation Doubling power multiplies both intensities by two, raising each level by 3.0103 dB. Their ratio and level difference remain unchanged, so the inferred height remains 17.32 m. The method eliminates unknown source power through the ratio. Physical check The farther slant distance is 34.64 m. The result depends on isotropic spreading; directivity could imitate a range-dependent level change.

Question 4

A level drop can determine an unknown geometric range

An isotropic point source is at height hh above a flat reference plane. One receiver is directly below it; another is 30.0m30.0\,\mathrm m horizontally away. The farther receiver measures 6.0206dB6.0206\,\mathrm{dB} less intensity level. Neglect reflections and absorption.

Diagram shown in the original SVG worksheet.

  1. Infer hh using spherical spreading.

  2. If the source power doubles, determine whether the inferred height or the level difference changes.

Question 4 - Solution

A level drop can determine an unknown geometric range

Diagram shown in the original SVG worksheet.

(a) Method and calculation

For equal source power, I∝1/r2I\propto1/r^2. The level difference givesInearIfar=106.0206/10=4.000,rfarrnear=2.\frac{I_{\mathrm{near}}}{I_{\mathrm{far}}}=10^{6.0206/10}=4.000,\quad\frac{r_{\mathrm{far}}}{r_{\mathrm{near}}}=2.h2+302=2h⇒3h2=900⇒h=17.32m.\sqrt{h^2+30^2}=2h\Rightarrow3h^2=900\Rightarrow h=17.32\,\mathrm m.

(b) Interpretation and further calculation

Doubling power multiplies both intensities by two, raising each level by 3.0103dB3.0103\,\mathrm{dB}. Their ratio and level difference remain unchanged, so the inferred height remains 17.32m17.32\,\mathrm m. The method eliminates unknown source power through the ratio.

Physical check

The farther slant distance is 34.64m34.64\,\mathrm m. The result depends on isotropic spreading; directivity could imitate a range-dependent level change.