Electromagnetic Induction Previous Year Questions — JEE Main Physics

28 past-year Electromagnetic Induction questions from JEE Main (Physics) — page 6.

Q46 (2026)

A simple pendulum made of mass 10 g and a metallic wire of length 10 cm is suspended vertically in a uniform magnetic field of 2 T. The magnetic field direction is perpendicular to the plane of oscillations of the pendulum. If the pendulum is released from an angle of $60^{\circ}$ with vertical, then maximum induced EMF between the point of suspension and point of oscillation is ____ mV. (Take $g = 10 \text{ m/s}^{2}$)
### Related Formula $$\varepsilon = \frac{1}{2} B\omega l^{2}$$ $$mgl(1 - \cos \theta) = \frac{1}{2}(ml^{2})\omega^{2}$$ ### Core Logic The metallic string of the pendulum cuts the perpendicular magnetic field lines as it swings. The induced EMF along the length of a rotating rod is maximum when its angular velocity $\omega$ is maximum. This maximum $\omega$ occurs at the lowest point of the swing. ### Step 1: Find Maximum Angular Velocity Using conservation of mechanical energy from extreme to mean position: $$mgl(1 - \cos 60^{\circ}) = \frac{1}{2} I \omega_{\max}^{2}$$ $$mgl\left(1 - \frac{1}{2}\right) = \frac{1}{2}(ml^{2})\omega_{\max}^{2}$$ $$\frac{1}{2}mgl = \frac{1}{2}ml^{2}\omega_{\max}^{2}$$ $$\omega_{\max} = \sqrt{\frac{g}{l}}$$ ### Step 2: Substitute Values Given $l = 10 \text{ cm} = 0.1 \text{ m}$ and $g = 10 \text{ m/s}^{2}$. $$\omega_{\max} = \sqrt{\frac{10}{0.1}} = \sqrt{100} = 10 \text{ rad/s}$$ ### Step 3: Calculate Maximum EMF $$\varepsilon_{\max} = \frac{1}{2} B \omega_{\max} l^{2}$$ $$\varepsilon_{\max} = \frac{1}{2} (2 \text{ T})(10 \text{ rad/s})(0.1 \text{ m})^{2}$$ $$\varepsilon_{\max} = 10 \times 0.01 = 0.1 \text{ V}$$ Convert to millivolts: $$\varepsilon_{\max} = 100 \text{ mV}$$ ### Pattern Recognition Sees: "pendulum wire in magnetic field" → It's just a rotating rod! EMF is $\frac{1}{2} B \omega l^2$. Find max $\omega$ via energy conservation at the lowest point. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Induction Class 11 Physics: Work, Energy and Power

Q41 (2026)

A circular loop of radius 7 cm is placed in uniform magnetic field of 0.2 T directed perpendicular to plane of loop. The loop is converted into a square loop in 0.5 s. The EMF induced in the loop is ____ mV.
  1. $6.6$
  2. $13.2$
  3. $8.25$
  4. $1.32$
### Related Formula $$\text{EMF} = \frac{\Delta \phi}{\Delta t} = B \frac{A_1 - A_2}{\Delta t}$$ ### Core Logic The magnetic field is constant, but the area changes as the circle deforms into a square. Length of the wire is conserved. Circumference of circular loop = $2\pi r \approx 14\pi \, \mathrm{cm}$. Side length of the new square loop: $$4a = 14\pi \implies a = \frac{7\pi}{2} \, \mathrm{cm}$$ ### Step 1: Calculate Change in Area $$\Delta A = A_{\text{circle}} - A_{\text{square}}$$ $$A_1 = \pi r^2 = \pi (7)^2 = 49\pi \, \mathrm{cm}^2$$ $$A_2 = a^2 = \left( \frac{7\pi}{2} \right)^2 = \frac{49\pi^2}{4} \, \mathrm{cm}^2$$ $$\Delta A = \left( 49\pi - \frac{49\pi^2}{4} \right) \times 10^{-4} \, \mathrm{m}^2$$ ### Step 2: Calculate Flux Change and EMF $$\Delta \phi = B \Delta A = 0.2 \left( 49\pi - \frac{49\pi^2}{4} \right) \times 10^{-4}$$ Using $\pi \approx 3.1415$: $49\pi \approx 153.938$ $\frac{49\pi^2}{4} \approx 120.89$ $\Delta A \approx 33.04 \times 10^{-4} \, \mathrm{m}^2$ Wait, taking standard approximations: $$\Delta \phi = 0.2 \times 33.07 \times 10^{-4} = 6.614 \times 10^{-4} \, \mathrm{Wb}$$ $$\text{EMF} = \frac{\Delta \phi}{\Delta t} = \frac{6.614 \times 10^{-4}}{0.5} = 13.228 \times 10^{-4} \, \mathrm{V}$$ $$\text{EMF} = 1.32 \, \mathrm{mV}$$ ### Pattern Recognition When a loop is deformed into a different shape, perimeter is conserved. For a given perimeter, a circle always encloses maximum area. Subtracting the new area from the old area immediately gives the $\Delta A$ driving the induced EMF. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Induction

Q42 (2026)

Suppose a long solenoid of 100 cm length, radius 2 cm having 500 turns per unit length, carries a current $I = 10 \sin (\omega t)$ A, where $\omega = 1000 \text{ rad/s}$ . A circular conducting loop (B) of radius 1 cm coaxially slid through the solenoid at a speed $v = 1 \text{ cm/s}$ . The r.m.s. current through the loop when the coil B is inserted 10 cm inside the solenoid is $\alpha/\sqrt{2} \mu\text{A}$ . The value of $\alpha$ is ____. [Resistance of the loop $= 10\Omega$ ]
  1. $197$
  2. $80$
  3. $280$
  4. $100$
### Related Formula $$\epsilon = - A \frac{dB}{dt}$$ $B = \mu_0 n I$ $$i_{\text{rms}} = \frac{\epsilon_{\text{rms}}}{R}$$ ### Core Logic Since the loop B is well inside the long solenoid (10 cm deep into a 100 cm length), the magnetic field is uniform across its cross-section and approximately equal to the ideal solenoid field $B = \mu_0 n I$. Here $n = 500$ turns/m. The sliding velocity $v$ just means it's moving through a uniform field region, so motional EMF does not contribute to the flux change; only the transformer EMF (time-varying $B$ field) creates the induced current. ### Step 1: Calculate Induced EMF $$I = I_0 \sin \omega t \implies \frac{dI}{dt} = I_0 \omega \cos \omega t$$ $$\epsilon = A \frac{dB}{dt} = A \mu_0 n \frac{dI}{dt} = (\pi r^2) \mu_0 n (I_0 \omega \cos \omega t)$$ ### Step 2: Calculate RMS Current Peak EMF $\epsilon_0 = \pi r^2 \mu_0 n I_0 \omega$. $$i_0 = \frac{\epsilon_0}{R} = \frac{\pi r^2 \mu_0 n I_0 \omega}{R}$$ $$i_{\text{rms}} = \frac{i_0}{\sqrt{2}} = \frac{\pi r^2 \mu_0 n I_0 \omega}{\sqrt{2} R}$$ ### Step 3: Numerical Substitution $$i_{\text{rms}} = \frac{\pi \times (10^{-2})^2 \times (4\pi \times 10^{-7}) \times 500 \times 10 \times 1000}{\sqrt{2} \times 10}$$ $$i_{\text{rms}} = \frac{\pi \times 10^{-4} \times 4\pi \times 10^{-7} \times 5 \times 10^6}{\sqrt{2} \times 10}$$ $$i_{\text{rms}} = \frac{20\pi^2 \times 10^{-6} \times 10}{\sqrt{2} \times 10} = \frac{20\pi^2}{\sqrt{2}} \times 10^{-6} \, \mathrm{A}$$ Using $\pi^2 \approx 9.87$, $20\pi^2 \approx 197.39$. Thus, $i_{\text{rms}} \approx \frac{197}{\sqrt{2}} \, \mu\mathrm{A}$. $\alpha = 197$. ### Pattern Recognition Motion parallel to uniform field lines inside an ideal solenoid induces no motional EMF. Only the time derivative of the AC current $\frac{dI}{dt}$ contributes to Faraday induction. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electromagnetic Induction Class 12 Physics: Alternating Current
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