Solenoids and Toroids — Question 6

Section 29-4 · Physics pages 4722–4723

Question 6 An ideal toroid has a stronger field at its inner edge than at its outer edge An ideal tightly wound air-core toroid has N=500 turns, current I=.400 A, inner radius a=.0800 m and outer radius b=.120 m. Approximate the windings by a continuous symmetric distribution. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. r b a Schematic; labels, not drawing lengths, specify the data. (a) Use Ampère law to find the field within the winding region and calculate its inner and outer edge magnitudes. (b) Find the fields in the central hole and outside the toroid under this idealization, explaining the enclosed currents.
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Question 6 - Solution An ideal toroid has a stronger field at its inner edge than at its outer edge r b a (a) Method and calculation 2πrB(r) = µ0NI ⇒B(r) = µ0NI 2πr (a < r < b). B(a) = .500 mT, B(b) = .333333 mT . (b) Interpretation and further calculation r < a : Ienc = 0; r > b : Ienc = NI −NI = 0. B = 0 in the hole and exterior by the ideal winding symmetry. Physical check Zero circulation alone would not establish a zero local field; the ideal toroidal symmetry is an essential part of the argument.

Question 6

An ideal toroid has a stronger field at its inner edge than at its outer edge

An ideal tightly wound air-core toroid has N=500 turns, current I=.400 A, inner radius a=.0800 m and outer radius b=.120 m. Approximate the windings by a continuous symmetric distribution. Use vacuum permeability μ0≃4π×10−7Tm/A\mu_0\simeq4\pi\times10^{-7}\,\mathrm{T\,m/A} where numerical values are needed.

Diagram shown in the original SVG worksheet.

  1. Use Ampère law to find the field within the winding region and calculate its inner and outer edge magnitudes.

  2. Find the fields in the central hole and outside the toroid under this idealization, explaining the enclosed currents.

Question 6 - Solution

An ideal toroid has a stronger field at its inner edge than at its outer edge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

2πrB(r)=μ0NI⇒B(r)=μ0NI2πr(a<r<b).2\pi rB(r)=\mu_0NI\Rightarrow\boxed{B(r)=\frac{\mu_0NI}{2\pi r}}\quad(a<r<b).B(a)=.500mT,B(b)=.333333mT.\boxed{B(a)=.500\,\mathrm{mT},\quad B(b)=.333333\,\mathrm{mT}}.

(b) Interpretation and further calculation

r<a:Ienc=0;r>b:Ienc=NI−NI=0.r<a:\ I_{\mathrm{enc}}=0;\quad r>b:\ I_{\mathrm{enc}}=NI-NI=0.B=0 in the hole and exteriorby the ideal winding symmetry.\boxed{B=0\text{ in the hole and exterior}}\quad\text{by the ideal winding symmetry}.

Physical check

Zero circulation alone would not establish a zero local field; the ideal toroidal symmetry is an essential part of the argument.