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04-BS-9 · May 2015

Question 5 of 8: Maximum and Minimum EMF of a Shrinking Loop

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

National Exams — May 2015 — 04-BS-9 Basic Electromagnetics. Three-hour, closed-book exam (approved Casio/Sharp calculator only). Aids given: $\varepsilon_0=8.85\times10^{-12}$ F/m, $\mu_0=4\pi\times10^{-7}$ H/m, $e=1.6\times10^{-19}$ C. Format: eight questions offered; any five constitute a complete paper and only the first five appearing in the answer book are marked. All eight are solved below for completeness.

Reference texts: Sadiku, Elements of Electromagnetics / Hayt & Buck, Engineering Electromagnetics — Coulomb's law and superposition, Gauss's law, Biot–Savart law, magnetic field of current sheets, Faraday's law, capacitance and field energy, mutual inductance; Young & Freedman, University Physics with Modern Physics — light propagation and reflection geometry.

Question 5: Maximum and Minimum EMF of a Shrinking Loop (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given.

QuantityValue
Field $B$ (uniform, vertical)$0.1$ T
Initial circumference $C_0$$30$ cm $=0.30$ m
Rate of shrinkage $dC/dt$$1$ cm/s $=0.01$ m/s (constant)

Find. The maximum and minimum EMF induced as the loop shrinks from $C_0$ to zero.

t=0, C=30 cm (max EMF) shrinking → C=0 (min EMF) B (vertical)
Loop circumference shrinks linearly from 30 cm to 0; EMF magnitude is proportional to the instantaneous circumference, so it is largest at t=0 and zero as the loop vanishes.

Approach. Express the loop area in terms of its circumference, $A=C^2/4\pi$, then apply Faraday's law $\varepsilon=-B\,dA/dt$ with $C(t)$ decreasing linearly.

  1. Rate of change of area in terms of $C$. $$A=\frac{C^2}{4\pi}\ \Rightarrow\ \frac{dA}{dt}=\frac{C}{2\pi}\frac{dC}{dt}$$ $$|\varepsilon(t)|=B\left|\frac{dA}{dt}\right|=\frac{B\,C(t)}{2\pi}\left|\frac{dC}{dt}\right|$$ Since $|dC/dt|$ is constant, $|\varepsilon(t)|$ is directly proportional to the instantaneous circumference $C(t)$, which decreases monotonically from $C_0$ to $0$.
  2. Maximum EMF (at $t=0$, $C=C_0$). $$\varepsilon_{\max}=\frac{B\,C_0}{2\pi}\frac{dC}{dt}=\frac{(0.1)(0.30)}{2\pi}(0.01)$$ $$\varepsilon_{\max}=\boxed{4.775\times10^{-5}\ \text{V}}$$
  3. Minimum EMF (as $C\to0$, loop fully wound down). $$\varepsilon_{\min}=\frac{B(0)}{2\pi}\frac{dC}{dt}=\boxed{0\ \text{V}}$$
QuantityResult
$\varepsilon_{\max}$ (at $t=0$)$4.775\times10^{-5}$ V
$\varepsilon_{\min}$ (as $C\to0$)$0$ V