Lenz's Law — Question 1

Section 30-3 · Physics pages 4792–4793

Question 1 The induced current need not reverse when the applied field crosses zero A fixed loop of area A and resistance R has normal +z out of the page. Its uniform applied field is Bz = B0(1 −t/T), with B0 and T positive. Neglect self-inductance. Bz out of page positive current: counterclockwise Schematic; labels, not drawing lengths, specify the data. (a) Find the current sense before and after t=T. (b) For A=.0200 square metre, B0=.300 T, T=.100 s and R=6.00 ohms, calculate its value.
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Question 1 - Solution The induced current need not reverse when the applied field crosses zero Bz out of page positive current: counterclockwise (a) Method and calculation ˙Φ = A ˙Bz = −AB0/T < 0. E = −˙Φ = AB0/T > 0 ⇒counterclockwise for both t < T and t > T . (b) Interpretation and further calculation i = AB0 RT = (.0200)(.300) (6.00)(.100) . i = .0100 A . Physical check The induced field opposes the change, not necessarily the instantaneous applied field.

Question 1

The induced current need not reverse when the applied field crosses zero

A fixed loop of area A and resistance R has normal +z out of the page. Its uniform applied field is Bz=B0(1−t/T)B_z=B_0(1-t/T), with B0 and T positive. Neglect self-inductance.

Diagram shown in the original SVG worksheet.

  1. Find the current sense before and after t=T.

  2. For A=.0200 square metre, B0=.300 T, T=.100 s and R=6.00 ohms, calculate its value.

Question 1 - Solution

The induced current need not reverse when the applied field crosses zero

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Φ̇=AḂz=−AB0/T<0.\dot\Phi=A\dot B_z=-AB_0/T<0.ℰ=−Φ̇=AB0/T>0⇒counterclockwise for both t<T and t>T.\mathcal E=-\dot\Phi=AB_0/T>0\Rightarrow\boxed{\text{counterclockwise for both }t<T\text{ and }t>T}.

(b) Interpretation and further calculation

i=AB0RT=(.0200)(.300)(6.00)(.100).i=\frac{AB_0}{RT}=\frac{(.0200)(.300)}{(6.00)(.100)}.i=.0100A.\boxed{i=.0100\,\mathrm A}.

Physical check

The induced field opposes the change, not necessarily the instantaneous applied field.