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A uniform magnetic field is restricted within a region of radius rr. The magnetic field changes with time at a rate dBdt\frac{dB}{dt}. Loop 1 of radius RR (R>rR > r) encloses the region rr and Loop 2 of radius RR is entirely outside the region of the magnetic field as shown in the figure. Then the electromotive force (emf) generated is:

A

Zero in loop 1 and zero in loop 2

B

dBdtπr2-\frac{dB}{dt}\pi r^2 in loop 1 and dBdtπr2-\frac{dB}{dt}\pi r^2 in loop 2

C

dBdtπr2-\frac{dB}{dt}\pi r^2 in loop 1 and zero in loop 2

D

2dBdtπr22\frac{dB}{dt}\pi r^2 in loop 1 and zero in loop 2

Step-by-Step Solution

According to Faraday's Law of Induction, the induced emf is given by ε=dΦBdt\varepsilon = -\frac{d\Phi_B}{dt} .

  1. Loop 1: This loop (Radius RR) encloses the cylindrical region of the magnetic field (Radius rr). Since the field BB exists only within radius rr, the total magnetic flux through Loop 1 is determined by the area of the magnetic field region, not the area of the loop itself. Flux Φ1=B×(Area of field)=B(πr2)\Phi_1 = B \times (\text{Area of field}) = B(\pi r^2). Induced emf ε1=ddt(Bπr2)=πr2dBdt\varepsilon_1 = -\frac{d}{dt}(B\pi r^2) = -\pi r^2 \frac{dB}{dt}.

  2. Loop 2: This loop is situated entirely outside the region of the magnetic field. Therefore, no magnetic field lines pass through it. Flux Φ2=0\Phi_2 = 0. Induced emf ε2=d(0)dt=0\varepsilon_2 = -\frac{d(0)}{dt} = 0.

Thus, a non-zero emf depends on the rate of change of field and the area of the field enclosed, while a loop enclosing no flux generates zero emf.

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