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Motional EMF and Applied Force
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A square conducting loop with side length $L$ and resistance $R$ is being pulled at constant velocity $v$ out of a region with uniform magnetic field $B$ (perpendicular to the plane of the loop, directed into the page). At the instant when half of the loop’s area remains within the field region, what is the magnitude of the net force required to maintain this constant velocity?

A

$$F = \frac{B^2 L^2 v}{R}$$

B

$$F = \frac{B^2 L^2 v}{2R}$$

C

$$F = BLv$$

D

$$F = \frac{B^2 L v}{R}$$

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