EASY
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Why do induced currents oppose the change in magnetic flux that causes them?
 

Important Questions on Electromagnetic Induction

HARD
A long solenoid of radius R carries a time t dependent current It=I0t1-t . A ring of radius 2R is placed coaxially near its middle. During the time interval 0t1, the induced current IR and the induced EMFVR in the ring change as:
HARD
 A circular insulated copper wire loop is twisted to form two loops of area A  and 2A as shown in the figure. At the point of crossing the wires remain electrically insulated from each other. The entire loop lies in the plane (of the paper). A uniform magnetic field B  points into the plane of the paper. At t = 0, the loop starts rotating about the common diameter as axis with a constant angular velocity in the magnetic field. Which of the following options is/are correct?
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MEDIUM
A very long solenoid of radius R is carrying current It=kte-αtk>0, as a function of time t0. Counterclockwise current is taken to be positive. A circular conducting coil of radius 2R is placed in the equitorial plane of the solenoid and concentric with the solenoid. The current induced in the outer coil is correctly depicted, as a function of time, by:
MEDIUM
The relation between the charge flow ΔQ through the circuit of resistance r and the change in the magnetic flux ΔϕB is
EASY

In a coil of resistance 100 Ω, a current is induced by changing the magnetic flux through it as shown in the figure. The magnitude of change in flux through the coil is:
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MEDIUM
A planar loop of wire rotates in a uniform magnetic field. Initially, at t=0 , the plane of the loop is perpendicular to the magnetic field. If it rotates with a period of 10 s about an axis in its plane then the magnitude of induced emf will be maximum and minimum, respectively at:
MEDIUM
A 800 turn coil of the effective area 0.05  m2 is kept perpendicular to the magnetic field 5×10-5  T. When the plane of the coil is rotated by 90o around any of its coplanar axis in 0.1 s, the emf induced in the coil will be:
EASY

The magnetic flux linked with a coil (in Wb) is given by the equation  ϕ=5t2+3t+16. The magnitude of induced emf in the coil at the fourth second will be:

MEDIUM
The figure shows a bar magnet and a metallic coil. Consider four situations. (I) Moving the magnet away from the coil. (II) Moving the coil towards the magnet. (III) Rotating the coil about the vertical diameter. (IV) Rotating the coil about its axis.

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An emf in the coil will be generated for the following situations.
EASY
A long solenoid of diameter 0.1 m has 2×104 turns per meter. At the centre of the solenoid, a coil of 100 turns and radius 0.01 m is placed with its axis coinciding with the solenoid axis. The current in the solenoid reduces at a constant rate to 0 A from 4 A in 0.05 s. If the resistance of the coil is 10π2 Ω, the total charge flowing through the coil during this time is
MEDIUM
A circular coil of radius 10 cm is placed in a uniform magnetic field of 3.0×10-5 T with its plane perpendicular to the field initially. It is rotated at constant angular speed about an axis along the diameter of coil and perpendicular to magnetic field so that it undergoes half of rotation in 0.2 s. The maximum value of EMF induced (in μV) in the coil will be close to the integer....
MEDIUM
A uniform magnetic field is restricted within a region of radius,  r. The magnetic field changes with time at a rate, dBdt. Loop one of radius R>r encloses the region, r and loop two of radius, R is outside the region of magnetic field as shown in the figure below. Then the emf generated is

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EASY

A small bar magnet is moved through a coil at constant speed from one end to the other. Which of the following series of observations will be seen on the galvanometer G attached across the coil?

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Three positions shown describe: (a) the magnet's entry (b) magnet is completely inside and (c) magnet's exit.
MEDIUM
At time t=0 magnetic field of 1000 Gauss is passing perpendicularly through the area defined by the closed loop shown in the figure. If the magnetic field reduces linearly to 500 Gauss, in the next 5s, then induced EMF in the loop is:
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HARD

A light disc made of aluminium (a nonmagnetic material) is kept horizontally and is free to rotate about its axis as shown in the figure. A strong magnet is held vertically at a point above the disc away from its axis. On revolving the magnet about the axis of the disc, the disc will (figure is schematic and not drawn to scale)

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EASY
The magnetic flux through a coil varies with time as ϕ=5t2+6t+9. The ratio of emf at t=3 s to t=0 s will be
EASY
A conducting circular loop is placed in a uniform magnetic field, B=0.025 T with its plane perpendicular to the loop. The radius of the loop is made to shrink at a constant rate of 1 mm s-1. The induced emf when the radius is 2 cm, is
HARD
A conducting metal circular-wire-loop of radius r is placed perpendicular to a magnetic field which varies with time as B=B0e-tτ, where B0 and τ are constants at time t=0. If the resistance of the loop is R, then the heat generated in the loop after a long time t is
EASY
A coil of cross-sectional area A having n turns is placed in a uniform magnetic field B. When it is rotated with an angular velocity ω, the maximum e.m.f. induced in the coil will be:
HARD
A conducting square frame of side a and a long straight wire carrying current I are located in the same plane as shown in the figure. The frame moves to the right with a constant velocity V. The e.m.f induced in the frame (when the centre of the frame is at a distance x from the wire) will be proportional to :
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