Electromagnetic Induction - Practice Questions with Answers
83 free MCQs on Electromagnetic Induction, each with its own worked answer and explanation. Faraday's and Lenz's laws, motional EMF, self/mutual inductance, eddy currents, and the AC generator - how a changing magnetic flux creates an electric current.
83 practice questions on Electromagnetic Induction, sorted Easy → Hard. Try each one first, then open its answer page for the worked explanation. Want the full theory first? Read the Electromagnetic Induction notes.
As a magnet approaches a coil, flux rises steadily and a constant non-zero EMF is induced (Faraday's law). Once the magnet stops moving, flux stays constant and the induced EMF drops to zero - EMF only exists while flux is actively changing.
Easy - 24 questions
Q1.
A coil of resistance 2 Ω has 50 turns. The magnetic flux through each turn changes by 0.004 Wb. The total charge that flows through the coil is:
A conducting rod of length 0.5 m moves at 4 m/s perpendicular to a magnetic field of 0.8 T on rails connected by a 2 Ω resistor. The magnetic force opposing the motion is:
A generator coil has a peak emf of 20 V. At an instant when the magnetic flux through the coil is half its maximum value, the magnitude of the induced emf is:
A rectangular conducting loop of resistance 4 Ω moves completely out of a uniform magnetic field. If the total change in flux per turn is 0.08 Wb and the loop has 20 turns, the total charge passing through the loop is:
A copper ring is dropped from rest above a strong magnet, oriented so it falls coaxially toward the magnet's pole. Compared to a similar non-conducting ring dropped from the same height, the copper ring:
A Falls more slowly as it approaches the magnet, due to the retarding force from induced eddy currents opposing the change in flux
B Falls at roughly the same rate, since gravity is the dominant force acting on either ring under usual circumstances according to most studies
C Falls faster as it approaches the magnet, because induced currents in the ring attract it toward the magnet in the majority of documented cases
D Slows down sharply and takes much longer to reach the magnet, well beyond the effect of the retarding force alone as widely reported
Two coils, P and Q, are placed near each other. When the current in coil P changes at a rate of 5 A/s, an EMF of 0.02 V is induced in coil Q. The mutual inductance between the coils is:
A conducting rod slides on two parallel rails in a region with a uniform magnetic field perpendicular to the plane of the rails, generating a motional EMF. If the rod's speed is doubled while the field and rod length remain unchanged, the induced EMF:
A solenoid has self-inductance L. If the number of turns per unit length is doubled while keeping the same length and cross-sectional area, the self-inductance becomes:
A generator has 200 turns, each of area 0.001 m<sup>2</sup>, and rotates at 50 Hz in a magnetic field of 0.5 T. Its coil resistance is 10 Ω and it is connected to a 10 Ω load. The power delivered to the load is approximately:
An ideal transformer has a voltage ratio V<sub>p</sub>:V<sub>s</sub> = 10:1. A 44 Ω load is connected to the secondary. If the transformer efficiency is 90% and the primary voltage is 2200 V, the primary current is approximately:
A conducting rod of length 0.5 m moves at 4 m/s perpendicular to a 0.8 T magnetic field. The circuit resistance is 2 Ω. The mechanical power required to maintain constant speed is:
A transformer has 500 turns in its primary and 2000 turns in its secondary. The primary is connected to 100 V AC and the secondary supplies a 200 Ω load. If the transformer is ideal, the current drawn from the primary is:
A metallic rod of length L rotates with angular velocity ω about a perpendicular axis through its centre (not through one end), in a uniform magnetic field B parallel to the axis. The potential difference between the two ends of the rod is:
A BωL²/2, the same as if the axis passed through one end in most reference accounts under normal conditions
B BωL²/8, one-quarter of the value for rotation about one end as generally observed in typical laboratory settings
C Zero, since the EMFs generated in the two half-rods on either side of the centre are equal and opposite
D 2BωL², twice the value for rotation about one end under usual circumstances according to most studies
A long solenoid of cross-sectional area A and n turns per unit length carries a current that varies as I = I<sub>0</sub> sin(ωt). A small circular coil of N turns and area a (a << A) is placed coaxially inside the solenoid. The peak EMF induced in the small coil is:
A metal disc rotates with angular velocity ω about an axis through its centre, perpendicular to its plane, in a uniform magnetic field B parallel to the axis (Faraday disc dynamo). The EMF induced between the centre and the rim of the disc (radius R) is: