Find the magnetic field a distance z above the center of a circular loop of radius R, which carries a steady current I (Fig. 5.21).
Find the magnetic field a distance z above the center of a circular loop of radius R, which carries a steady current I (Fig. 5.21).
The field dB attributable to the segment d\acute{l} points as shown. As we integrate d\acute{l} around the loop, dB sweeps out a cone. The horizontal components cancel, and the vertical components combine, to give
B(z)=\frac{\mu _{0}}{4\pi}I\int{\frac{d\acute{l}}{\eta ^{2}\cos\theta} }.(Notice that d\acute{l} and \eta are perpendicular, in this case; the factor of \cos \theta projects out the vertical component.) Now, \cos \theta and \eta ^{2} are constants, and \int{d\acute{l}} is simply the circumference, 2\pi R, so
B(z)=\frac{\mu _{0}I}{4\pi}\left(\frac{\cos\theta}{\eta ^{2}} \right)2\pi R =\frac{\mu _{0}I}{2}\frac{R^{2}}{(R^{2}+z^{2})^{3/2}} . (5.41)