Difficulty distribution
How the classified questions are distributed by difficulty.
Your cart is empty.
Practice Electromagnetic Induction - Electromagnetism - Physics previous year questions organised from real papers, with year-wise coverage and clear topic navigation.
Every graph below is calculated only from this selection.
Year-wise coverage for Electromagnetic Induction. Each bar uses a separate theme-derived color.
How the classified questions are distributed by difficulty.
MCQ, numerical, multiple-select and other formats found in these papers.
Top subjects by unique question coverage.
Top topics across the included previous year papers.
Top subtopics inside this exact selection.
Question coverage for the most populated papers. Every active PYP paper remains listed below.
Newest papers appear first. Sort by year, question coverage or name.
| Paper | Year / session | Questions in this view | Open |
|---|---|---|---|
| MHT CET 2026 11th April Evening Shift | 2026 | 2 | View paper |
| MHT CET 2026 11th April Morning Shift | 2026 | 3 | View paper |
| MHT CET 2026 13th April Evening Shift | 2026 | 2 | View paper |
| MHT CET 2026 13th April Morning Shift | 2026 | 2 | View paper |
| MHT CET 2026 15th April Evening Shift | 2026 | 2 | View paper |
| MHT CET 2026 15th April Morning Shift | 2026 | 3 | View paper |
| MHT CET 2026 16th April Evening Shift | 2026 | 3 | View paper |
| MHT CET 2026 16th April Morning Shift | 2026 | 1 | View paper |
| MHT CET 2026 17th April Evening Shift | 2026 | 3 | View paper |
| MHT CET 2026 17th April Morning Shift | 2026 | 2 | View paper |
| MHT CET 2026 18th April Evening Shift | 2026 | 3 | View paper |
| MHT CET 2026 18th April Morning Shift | 2026 | 3 | View paper |
| MHT CET 2026 19th April Evening Shift | 2026 | 2 | View paper |
| MHT CET 2026 19th April Morning Shift | 2026 | 3 | View paper |
| MHT CET 2026 20th April Evening Shift | 2026 | 2 | View paper |
| MHT CET 2026 20th April Morning Shift | 2026 | 2 | View paper |
| MHT CET (PCB) 2025 9th April Evening Shift | 2025 | 2 | View paper |
| MHT CET (PCB) 2025 9th April Morning Shift | 2025 | 3 | View paper |
| MHT CET 2025 19TH APRIL EVENING SHIFT | 2025 | 2 | View paper |
| MHT CET 2025 19TH APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 20TH APRIL EVENING SHIFT | 2025 | 2 | View paper |
| MHT CET 2025 20TH APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 21ST APRIL EVENING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 21ST APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 22ND APRIL EVENING SHIFT | 2025 | 1 | View paper |
| MHT CET 2025 22ND APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 23RD APRIL EVENING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 23RD APRIL MORNING SHIFT | 2025 | 2 | View paper |
| MHT CET 2025 25TH APRIL EVENING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 25TH APRIL MORNING SHIFT | 2025 | 1 | View paper |
| MHT CET 2025 26TH APRIL EVENING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 26TH APRIL MORNING SHIFT | 2025 | 3 | View paper |
| MHT CET 2025 5TH MAY EVENING SHIFT | 2025 | 3 | View paper |
| MHT CET (PCB) 2024 22th April Evening Shift | 2024 | 2 | View paper |
| MHT CET (PCB) 2024 22th April Morning Shift | 2024 | 2 | View paper |
| MHT CET 2024 10TH MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 10TH MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 11TH MAY EVENING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 11TH MAY MORNING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 15TH MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 15TH MAY MORNING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 16TH MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 16TH MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 2ND MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 2ND MAY MORNING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 3RD MAY EVENING SHIFT | 2024 | 2 | View paper |
| MHT CET 2024 3RD MAY MORNING SHIFT | 2024 | 1 | View paper |
| MHT CET 2024 4TH MAY EVENING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 4TH MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 9TH MAY EVENING SHIFT | 2024 | 3 | View paper |
| MHT CET 2024 9TH MAY MORNING SHIFT | 2024 | 3 | View paper |
| MHT CET 2023 10TH MAY EVENING SHIFT | 2023 | 2 | View paper |
| MHT CET 2023 10TH MAY MORNING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 11TH MAY EVENING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 11TH MAY MORNING SHIFT | 2023 | 4 | View paper |
| MHT CET 2023 12TH MAY EVENING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 12TH MAY MORNING SHIFT | 2023 | 2 | View paper |
| MHT CET 2023 13TH MAY EVENING SHIFT | 2023 | 2 | View paper |
| MHT CET 2023 13TH MAY MORNING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 14TH MAY EVENING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 14TH MAY MORNING SHIFT | 2023 | 2 | View paper |
| MHT CET 2023 9TH MAY EVENING SHIFT | 2023 | 3 | View paper |
| MHT CET 2023 9TH MAY MORNING SHIFT | 2023 | 4 | View paper |
| MHT CET 2022 11TH AUGUST EVENING SHIFT | 2022 | 3 | View paper |
| MHT CET 2021 20TH SEPTEMBER EVENING SHIFT | 2021 | 1 | View paper |
| MHT CET 2021 20TH SEPTEMBER MORNING SHIFT | 2021 | 2 | View paper |
| MHT CET 2021 21TH SEPTEMBER MORNING SHIFT | 2021 | 3 | View paper |
| MHT CET 2021 22TH SEPTEMBER EVENING SHIFT | 2021 | 1 | View paper |
| MHT CET 2021 22TH SEPTEMBER MORNING SHIFT | 2021 | 2 | View paper |
| MHT CET 2021 23RD SEPTEMBER EVENING SHIFT | 2021 | 3 | View paper |
| MHT CET 2021 23th September Morning Shift | 2021 | 3 | View paper |
| MHT CET 2021 24TH SEPTEMBER EVENING SHIFT | 2021 | 3 | View paper |
| MHT CET 2021 24TH SEPTEMBER MORNING SHIFT | 2021 | 2 | View paper |
| MHT CET 2020 16TH OCTOBER EVENING SHIFT | 2020 | 1 | View paper |
| MHT CET 2020 16TH OCTOBER MORNING SHIFT | 2020 | 1 | View paper |
| MHT CET 2020 19TH OCTOBER EVENING SHIFT | 2020 | 1 | View paper |
| MHT CET 2019 2ND MAY MORNING SHIFT | 2019 | 1 | View paper |
Practice every matching question in batches of 20, with every available option.
2. Two coils have a mutual inductance of 0.01 H . The current in the first coil changes according to equation, $I=5 \sin 200 \pi t$. The maximum value of emf induced in the second coil is
The length of solenoid is \(I\) whose windings are made of material of density \(D\) and resistivity \(\rho\). The winding resistance is \(R\). The inductance of solenoid is [\(m=\) mass of winding wire, \(\mu_0=\) permeability of free space]
A coil of \(n\) turns and resistance \(R \Omega\) is connected in series with a resistance \(\frac{R}{2}\). The combination is moved for time \(t\) second through magnetic flux \(\phi_1\) to \(\phi_2\). The induced current in the circuit is
Metal rings $P$ and $Q$ are lying in the same plane, where current I is increasing steadily. The induced current in metal rings is shown correctly in figure

A metal wire of length \(2500 \mathrm{~m}\) is kept in east-west direction, at a height of \(10 \mathrm{~m}\) from the ground. If it falls freely on the ground then the current induced in the wire is (Resistance of wire \(=25 \sqrt{2} \Omega, \mathrm{g}=10 \mathrm{~m} / \mathrm{s}^2\) and Earth's horizontal component of magnetic field \(\left.\mathrm{B}_{\mathrm{H}}=2 \times 10^{-5} \mathrm{~T}\right)\)
Two conducting wire loops are concentric and lie in the same plane. The current in the outer loop is clockwise and increasing with time. The induced current in the inner loop is
A straight conductor of length 0.6 M is moved with a speed of 10 ms\(^{-1}\) perpendicular to magnetic field of induction 1.2 weber m\(^{-2}\). The induced e.m.f. across the conductor is
A wire of length '\(L\)'; having resistance '\(R\)' falls from a height '\(\ell\)' in earth's horizontal magnetic field '\(B\)'. The current through the wire is ( \(\mathrm{g}=\) acceleration due to gravity)
A coil of radius '\(\mathrm{r}\)' is placed on another coil (whose radius is '\(\mathrm{R}\)' and current through it is changing) so that their centres coincide. ( \(R > r\) ). If both coplanar, then the mutual inductance between them is proportional to
The magnetic potential energy stored in a certain inductor is \(25 \mathrm{~mJ}\), when the current in the inductor is \(50 \mathrm{~mA}\). This inductor is of inductance
the magnetic flux (in weber) in a closed circuit of resistance \(20 \Omega\) varies with time \(t\) second according to equation \(\phi=5 t^2-6 t+9\). The magnitude of induced current at \(t=0.2\) second is
A circular coil of radius '\(R\)' has '\(N\)' turns of a wire. The coefficient of self induction of the coil will be ( \(\mu_0=\) permeability of free space)
A wire of length 1 m is moving at a speed of 2 m/s perpendicular homogenous magnetic field of 0.5 T. The ends of the wire are joined to resistance 6\(\Omega\). The rate at which work is being done to keep the wire moving at that speed is
A conducting loop of resistance 'R' is moved to magnetic field, the total induced charge depends upon
The self inductance of solenoid of length \(31.4 \mathrm{~cm}\), area of cross section \(10^{-3} \mathrm{~m}^2\) having total number of turns 500 will be nearly [\(\mu_0=4 \pi \times 10^{-7}\) SI unit]
A circuit has self-inductance 'L' H and carries a current 'I' A. To prevent sparking when the circuit is switched off, a capacitor which can withstand 'V' volt is used. The least capacitance of the capacitor connected across the switch must be equal to
A rectangular loop \(\mathrm{PQMN}\) with movable arm \(\mathrm{PQ}\) of length \(12 \mathrm{~cm}\) and resistance \(2 \Omega\) is placed in a uniform magnetic field of \(0.1 \mathrm{~T}\) acting perpendicular to the plane of the loop as shown in figure. The resistances of the arms MN, NP and MQ are negligible. The current induced in the loop when arm PQ is moved with velocity \(20 \mathrm{~ms}^{-1}\) is

A current \(I=10 \sin (100 \pi t)\) ampere, is passed in a coil which induces a maximum emf \(5 \pi\) volt in neighbouring coil. The mutual inductance of two coils is
A current 'I' produces a magnetic flux '\(\phi\)' per turn in a coil of '\(n\)' turns. Self inductance of the coil is '\(L\)'. The relation between them is
. If the current of '\(I\)' A gives rise to a magnetic flux '\(\phi\)' through a coil having '\(N\)' turns then mangetic energy stored in the medium surrounding the coil is
Showing 20 of 184 questions