Faraday's Law Need help with explanation

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SUMMARY

The discussion focuses on Faraday's Law and the induced electromotive force (emf) in three wire-loop configurations due to a sinusoidal current I=Io cos wt. Configuration (a), which lies in the y-z plane, induces the largest emf because the magnetic field generated by the current penetrates the loop area at a 90-degree angle, allowing for a maximum rate of change of magnetic flux. In contrast, configurations (b) and (c) lie in the x-y plane, where the magnetic field is parallel to the loop, resulting in zero flux change and no induced emf. The relationship ε = -dψ/dt is crucial in understanding this phenomenon.

PREREQUISITES
  • Understanding of Faraday's Law of Electromagnetic Induction
  • Familiarity with magnetic fields and their interaction with current-carrying conductors
  • Knowledge of sinusoidal functions and their properties
  • Basic grasp of vector calculus as it applies to electromagnetism
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  • Study the implications of Faraday's Law in different geometrical configurations of loops
  • Explore the concept of magnetic flux and its calculation in various scenarios
  • Learn about the right-hand rule for determining the direction of magnetic fields
  • Investigate applications of induced emf in real-world electrical systems
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Homework Statement



http://em.groups.et.byu.net/embook/ch6/mod6.4.html

^^The link has the problem
Three wire-loop configurations are shown below. In all cases, the long straight wire is oriented along the z-direction and carried current I=Io cos wt. The loop in (a) lies in the y-z plane. In contrast, the loops in (b) and (c) lie in the x-y plane. All three loops are of equal area. Explain which loop configuration will induce a V emf with the largest amplitude.

Homework Equations





The Attempt at a Solution



I know the answer is (a), but can someone explain to me the reason configuration (A) induces the largest V emf?? compared to (b) or (c)??
 
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The emf induced is proportional to the rate of change of flux penetrating the area of the loop.

ε = - dψ/dt
(which comes from ∇×E = -∂B/dt integrated over the area enclosed by the loop)

The current I sets up a magnetic field that circles the wire. Take your right hand, point your thumb in the direction of the current and your folded fingers show you how the magnetic field circles the wire.

For b and c, the field is parallel to the plane containing the wire loop so no flux passes through the area enclosed by the loop. ∂ψ/dt is zero so no emf is induced.

For a, the field penetrates the loop area at 90 degrees. Because the current is sinusoidal and the B it generates is proportional to the current, the B penetrating the loop is also sinusoidal, ie is changing. Therefore an emf is induced in the loop.
 

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