A conducting square loop of side $L$ and resistance $R$ moves in its plane with a uniform velocity $v$ perpendicular to one of its sides. A magnetic induction $B$ , constant in time and space, pointing perpendicular and into the plane of the lop exists everywhere.
The current induced in the loop is

B L v / R

clockwise

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B L v / R

anticlockwise

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2 B L v / R

anticlockwise

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zero

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Solution

The correct option is C zero
According to Faraday's law
Voltage is induced due to change in the magnetic flux through a closed loop.
Here
Magnetic Flux = $ϕ = B A = c o n s t .$
Hence
Induced EMF = $\frac{d ϕ}{d t} = 0$
Induced current = $i = E / R = 0$

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A conducting square loop of side L and resistance R moves in its plane with a uniform velocity v perpendicular to one of its sides. A magnetic induction B, constant in time and space, pointing perpendicular and into the plane of the lop exists everywhere.The current induced in the loop is

The correct option is C zeroAccording to Faraday's lawVoltage is induced due to change in the magnetic flux through a closed loop.Here Magnetic Flux = ϕ=BA=const.HenceInduced EMF = dϕdt=0Induced current =i=E/R=0

A conducting square loop of side $L$ and resistance $R$ moves in its plane with a uniform velocity $v$ perpendicular to one of its sides. A magnetic induction $B$ , constant in time and space, pointing perpendicular and into the plane of the lop exists everywhere.
The current induced in the loop is

The correct option is C zero
According to Faraday's law
Voltage is induced due to change in the magnetic flux through a closed loop.
Here
Magnetic Flux = $ϕ = B A = c o n s t .$
Hence
Induced EMF = $\frac{d ϕ}{d t} = 0$
Induced current = $i = E / R = 0$