A toroid whose dimensions are shown in Figure 7.15 has N turns and carries current I. Determine H inside and outside the toroid.
A toroid whose dimensions are shown in Figure 7.15 has N turns and carries current I. Determine H inside and outside the toroid.
We apply Ampère’s circuit law to the Amperian path, which is a circle of radius \rho shown dashed in Figure 7.15. Since N wires cut through this path each carrying current I, the net current enclosed by the Amperian path is NI. Hence,
\oint H\cdot dl=I_{enc}\rightarrow H\cdot 2\pi\rho=NI
or
H=\frac{NI}{2\pi\rho}, for \rho_{o}-a\lt \rho\lt \rho_{o}+a
where \rho_{o} is the mean radius of the toroid as shown in Figure 7.15. An approximate value of H is
H_{approx}=\frac{NI}{2\pi\rho_{o}}=\frac{NI}{\ell}
Notice that this is the same as the formula obtained for H for points well inside a very long solenoid (\ell\gg a). Thus a straight solenoid may be regarded as a special toroidal coil for which \rho_{o}\rightarrow\infty . Outside the toroid, the current enclosed by an Amperian path is NI-NI=0 and hence H=0.