Energy Transport and the Poynting Vector — Question 2

Section 33-4 · Physics pages 5434–5435

Question 2 Spherical spreading reduces intensity faster than field amplitude An ideal isotropic source radiates total electromagnetic power P in vacuum. A small detector is far enough away for a locally plane wave. There is no absorption. r equal power through each sphere Schematic; labels, not drawing lengths, specify the data. (a) Derive the distance dependence of intensity and rms electric field. (b) If rms field drops from E1 to E1/3 while the source power is unchanged, find the distance ratio and the intensity ratio.
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Question 2 - Solution Spherical spreading reduces intensity faster than field amplitude r equal power through each sphere (a) Method and calculation I(r) = P 4πr2 , Erms = √ I/(ϵ0c). Erms(r) = 1 r √ P 4πϵ0c . (b) Interpretation and further calculation E2/E1 = r1/r2 = 1/3 ⇒r2/r1 = 3 . I2/I1 = (r1/r2)2 = 1/9 . Physical check The same total power crosses every concentric sphere; field amplitude scales as the square root of intensity.

Question 2

Spherical spreading reduces intensity faster than field amplitude

An ideal isotropic source radiates total electromagnetic power P in vacuum. A small detector is far enough away for a locally plane wave. There is no absorption.

Diagram shown in the original SVG worksheet.

  1. Derive the distance dependence of intensity and rms electric field.

  2. If rms field drops from E1 to E1/3 while the source power is unchanged, find the distance ratio and the intensity ratio.

Question 2 - Solution

Spherical spreading reduces intensity faster than field amplitude

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I(r)=P4πr2,Erms=I/(ϵ0c).I(r)=\frac{P}{4\pi r^2},\quad E_{\mathrm{rms}}=\sqrt{I/(\epsilon_0c)}.Erms(r)=1rP4πϵ0c.\boxed{E_{\mathrm{rms}}(r)=\frac1r\sqrt{\frac{P}{4\pi\epsilon_0c}}}.

(b) Interpretation and further calculation

E2/E1=r1/r2=1/3⇒r2/r1=3.E_2/E_1=r_1/r_2=1/3\Rightarrow\boxed{r_2/r_1=3}.I2/I1=(r1/r2)2=1/9.\boxed{I_2/I_1=(r_1/r_2)^2=1/9}.

Physical check

The same total power crosses every concentric sphere; field amplitude scales as the square root of intensity.