Two Experiments — Question 8

Section 30-1 · Physics pages 4766–4767

Question 8 A slotted pickup interrupts conduction without removing the changing flux Two otherwise identical pickup loops surround the same changing source. Loop A is closed with resistance R; loop B has a narrow insulating gap. An ideal high-impedance detector spans the gap with leads routed together. The supplied loop emf magnitude is E. B(t) out of page positive current: counterclockwise gap and detector Schematic; labels, not drawing lengths, specify the data. (a) Compare the steady quasistatic conduction currents and resistive heating. (b) For finite detector resistance Rm much greater than R, estimate the gap voltage and the loading error.
Show solutionHide solution
Question 8 - Solution A slotted pickup interrupts conduction without removing the changing flux B(t) out of page positive current: counterclockwise gap and detector (a) Method and calculation |iA| = E/R, PA = E2/R. Rm →∞: iB →0, PB →0 . (b) Interpretation and further calculation iB = E R + Rm , |Vm| = ERm R + Rm . E −|Vm| E = R R + Rm ≃R/Rm . Physical check The gap does not eliminate the induced emf. The stated voltage assumes tightly paired measurement leads and the prescribed flux-linking contour.

Question 8

A slotted pickup interrupts conduction without removing the changing flux

Two otherwise identical pickup loops surround the same changing source. Loop A is closed with resistance R; loop B has a narrow insulating gap. An ideal high-impedance detector spans the gap with leads routed together. The supplied loop emf magnitude is E.

Diagram shown in the original SVG worksheet.

  1. Compare the steady quasistatic conduction currents and resistive heating.

  2. For finite detector resistance Rm much greater than R, estimate the gap voltage and the loading error.

Question 8 - Solution

A slotted pickup interrupts conduction without removing the changing flux

Diagram shown in the original SVG worksheet.

(a) Method and calculation

|iA|=E/R,PA=E2/R.|i_A|=E/R,\quad P_A=E^2/R.Rm→∞:iB→0,PB→0.R_m\to\infty:\quad\boxed{i_B\to0,\ P_B\to0}.

(b) Interpretation and further calculation

iB=ER+Rm,|Vm|=ERmR+Rm.i_B=\frac E{R+R_m},\quad |V_m|=\frac{ER_m}{R+R_m}.E−|Vm|E=RR+Rm≃R/Rm.\boxed{\frac{E-|V_m|}{E}=\frac R{R+R_m}\simeq R/R_m}.

Physical check

The gap does not eliminate the induced emf. The stated voltage assumes tightly paired measurement leads and the prescribed flux-linking contour.