Solenoids and Toroids — Question 8

Section 29-4 · Physics pages 4726–4727

Question 8 Reversed turns reduce a toroidal field twice as much as inactive turns A toroidal winding is intended to have N=200 turns all carrying I with the same orientation. In an idealized distributed winding, k=5 turns are instead reversed while carrying the same current. Keep the geometry and current magnitude fixed; neglect leakage. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. r b a signed enclosed ampere-turns Schematic; labels, not drawing lengths, specify the data. (a) Find the field relative to its intended value and the current correction needed to restore that value. (b) Compare with five electrically bypassed, inactive turns and explain the factor-of-two difference in field loss.
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Question 8 - Solution Reversed turns reduce a toroidal field twice as much as inactive turns r b a signed enclosed ampere-turns (a) Method and calculation NI actual = (N −k)I −kI = (N −2k)I. B/B0 = 190/200 = .950, I′/I = 200/190 = 20/19 . (b) Interpretation and further calculation inactive turns: B/B0 = (N −k)/N = 195/200 = .975. ∆Breversed/B0 = 2k/N, ∆Binactive/B0 = k/N . Physical check A reversed turn removes its intended positive contribution and adds an equal negative contribution. This model concerns linked ampere-turns, not localized leakage near an individual defective turn.

Question 8

Reversed turns reduce a toroidal field twice as much as inactive turns

A toroidal winding is intended to have N=200 turns all carrying I with the same orientation. In an idealized distributed winding, k=5 turns are instead reversed while carrying the same current. Keep the geometry and current magnitude fixed; neglect leakage. 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. Find the field relative to its intended value and the current correction needed to restore that value.

  2. Compare with five electrically bypassed, inactive turns and explain the factor-of-two difference in field loss.

Question 8 - Solution

Reversed turns reduce a toroidal field twice as much as inactive turns

Diagram shown in the original SVG worksheet.

(a) Method and calculation

NI|actual=(N−k)I−kI=(N−2k)I.NI\big|_{\mathrm{actual}}=(N-k)I-kI=(N-2k)I.B/B0=190/200=.950,I′/I=200/190=20/19.\boxed{B/B_0=190/200=.950,\quad I\prime/I=200/190=20/19}.

(b) Interpretation and further calculation

inactive turns:B/B0=(N−k)/N=195/200=.975.\text{inactive turns:}\quad B/B_0=(N-k)/N=195/200=.975.ΔBreversed/B0=2k/N,ΔBinactive/B0=k/N.\boxed{\Delta B_{\mathrm{reversed}}/B_0=2k/N,\quad\Delta B_{\mathrm{inactive}}/B_0=k/N}.

Physical check

A reversed turn removes its intended positive contribution and adds an equal negative contribution. This model concerns linked ampere-turns, not localized leakage near an individual defective turn.