An even more useful way to express the energy carried by an electromagnetic wave is in terms of the wave intensity, or average power per unit area. Figure 22-12 shows a portion of a wave that has cross-sectional area \(A\) and length \(\ell\). The energy in this portion of the wave is \(u_{\mathrm{average}}\) from Equation 22-24 multiplied by the volume \(A\ell\) of this portion. This entire portion of the wave moves at speed \(c\) through the cross-sectional area \(A\) in a time \(t\). The power equals the energy in the wave portion divided by the time \(t = \ell/c\) that it takes this portion of the wave to travel at speed c through the crosssectional area \(A\). The intensity, to which we give the symbol \(S_{\mathrm{average}}\), equals the power divided by the area \(A\). So
\(S_{\mathrm{average}}= \frac{\mathrm{energy}}{\mathrm{time}} \times \frac{1}{\mathrm{area}} = \frac{(u_{\mathrm{average}}A \ell)}{\ell /c} \times \frac{1}{A} = u_{\mathrm{average}}c\)
Using Equation 22-24, we can rewrite this as
(To write the last expression in Equation 22-25, we used the result that since \(B_0 = E_0/c\), it follows that \(B_{\mathrm{rms}} = E_{\mathrm{rms}}/c\).)