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Chapter 4

Current Electricity and Magnetism

MBBS and BDS entrance past exam questions

Past questions and answers

72 questions set from this chapter. Most repeated first.

  • 2013 · NEET-UG (India) · 4 marks

A wire of resistance 4 Ω4\ \Omega is stretched to twice its original length. The resistance of stretched wire would be:
(a) 2 Ω2\ \Omega (b) 4 Ω4\ \Omega (c) 8 Ω8\ \Omega (d) 16 Ω16\ \Omega

Answer

(d) 16 Ω16\ \Omega

Stretching keeps volume constant, so doubling the length halves the area. Since R=ρlAR=\rho\frac{l}{A}, resistance becomes 2×2=42\times2=4 times. New resistance =4×4=16 Ω=4\times4=16\ \Omega.

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  • 2013 · NEET-UG (India) · 4 marks

The internal resistance of a 2.1 V cell which gives a current of 0.2 A through a resistance of 10 Ω10\ \Omega is:
(a) 0.2 Ω0.2\ \Omega (b) 0.5 Ω0.5\ \Omega (c) 0.8 Ω0.8\ \Omega (d) 1.0 Ω1.0\ \Omega

Answer

(b) 0.5 Ω0.5\ \Omega

ε=I(R+r)\varepsilon=I(R+r), so R+r=2.10.2=10.5 ΩR+r=\frac{2.1}{0.2}=10.5\ \Omega. Therefore r=10.5−10=0.5 Ωr=10.5-10=0.5\ \Omega.

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  • 2013 · NEET-UG (India) · 4 marks

When a proton is released from rest in a room, it starts with an initial acceleration a0a_0 towards west. When it is projected towards north with a speed v0v_0 it moves with an initial acceleration 3a03a_0 toward west. The electric and magnetic fields in the room are:
(a) ma0e\frac{ma_0}{e} west, 2ma0ev0\frac{2ma_0}{ev_0} up (b) ma0e\frac{ma_0}{e} west, 2ma0ev0\frac{2ma_0}{ev_0} down (c) ma0e\frac{ma_0}{e} east, 3ma0ev0\frac{3ma_0}{ev_0} up (d) ma0e\frac{ma_0}{e} east, 3ma0ev0\frac{3ma_0}{ev_0} down

Answer

(b) ma0e\frac{ma_0}{e} west, 2ma0ev0\frac{2ma_0}{ev_0} down

At rest only the electric force acts: eE=ma0eE=ma_0 westward, so E=ma0eE=\frac{ma_0}{e} west (proton is positive). Moving north, the acceleration is 3a03a_0 west, so the magnetic force adds 2ma02ma_0 west: ev0B=2ma0ev_0B=2ma_0. With F⃗=ev⃗×B⃗\vec F=e\vec v\times\vec B, north ×\times down gives west, so BB points down.

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  • 2013 · NEET-UG (India) · 4 marks

A current loop in a magnetic field:
(a) experiences a torque whether the field is uniform or non-uniform in all orientations (b) can be in equilibrium in one orientation (c) can be in equilibrium in two orientations, both the equilibrium states are unstable (d) can be in equilibrium in two orientations, one stable while the other is unstable

Answer

(d) can be in equilibrium in two orientations, one stable while the other is unstable

Torque τ⃗=m⃗×B⃗\vec\tau=\vec m\times\vec B vanishes when m⃗\vec m is parallel (stable) or antiparallel (unstable) to B⃗\vec B. So there are two equilibrium orientations. A loop does not always experience a torque (it is zero in these two orientations), which rules out (a).

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  • 2013 · NEET-UG (India) · 4 marks

A bar magnet of length ll and magnetic dipole moment MM is bent in the form of an arc (subtending 60∘60^\circ at its centre) as shown in figure. The new magnetic dipole moment will be:
(a) MM (b) 3πM\frac{3}{\pi}M (c) 2πM\frac{2}{\pi}M (d) M2\frac{M}{2}

Answer

(b) 3πM\frac{3}{\pi}M

Dipole moment is pole strength times distance between poles, M=mlM=ml. Bent into an arc of 60∘60^\circ, the arc length stays ll, so the radius is r=lπ/3=3lπr=\frac{l}{\pi/3}=\frac{3l}{\pi}. The poles are now separated by the chord =2rsin⁡30∘=r=3lπ=2r\sin30^\circ=r=\frac{3l}{\pi}, so M′=m⋅3lπ=3πMM'=m\cdot\frac{3l}{\pi}=\frac{3}{\pi}M.

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  • 2013 · NEET-UG (India) · 4 marks

A wire loop is rotated in a magnetic field. The frequency of change of direction of the induced e.m.f. is:
(a) once per revolution (b) twice per revolution (c) four times per revolution (d) six times per revolution

Answer

(b) twice per revolution

The induced emf e=e0sin⁡ωte=e_0\sin\omega t changes sign each time the loop passes the neutral position (plane perpendicular to the field). That happens twice in each revolution, i.e. once every half cycle.

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  • 2014 · NEET-UG (India) · 4 marks

The resistances in the two arms of the meter bridge are 5 Ω5\ \Omega and R ΩR\ \Omega, respectively (the 5 Ω5\ \Omega resistance is in the left gap and RR in the right gap, with the balance length l1l_1 measured from end A). When the resistance RR is shunted with an equal resistance, the new balance point is at 1.6 l11.6\,l_1. The resistance RR is:
(a) 15 Ω15\ \Omega (b) 20 Ω20\ \Omega (c) 25 Ω25\ \Omega (d) 10 Ω10\ \Omega

Answer

(a) 15 Ω15\ \Omega

Balance condition: 5R=l1100−l1\frac5R=\frac{l_1}{100-l_1}. After shunting, the right arm is R2\frac R2: 10R=1.6l1100−1.6l1\frac{10}{R}=\frac{1.6l_1}{100-1.6l_1}. Dividing: 2=1.6(100−l1)100−1.6l12=\frac{1.6(100-l_1)}{100-1.6l_1}, giving l1=25l_1=25 cm. Then 5R=2575\frac5R=\frac{25}{75}, so R=15 ΩR=15\ \Omega.

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  • 2014 · NEET-UG (India) · 4 marks

A thin semicircular conducting ring (PQR) of radius rr is falling with its plane vertical in a horizontal magnetic field BB (directed into the plane of the ring), with P and R the ends of the ring and Q the top point. The potential difference developed across the ring when its speed is vv, is:
(a) Bvπr2/2Bv\pi r^2/2 and P is at higher potential (b) πrBv\pi r B v and R is at higher potential (c) 2rBv2rBv and R is at higher potential (d) Zero

Answer

(c) 2rBv2rBv and R is at higher potential

Only the chord joining the ends matters: the motional emf equals that of a straight conductor of length 2r2r moving perpendicular to BB, so ε=B(2r)v\varepsilon = B(2r)v. By v⃗×B⃗\vec v\times\vec B, positive charges are pushed towards R, so R is at higher potential. Option (b) wrongly uses the arc length πr\pi r; the emf depends on the effective (chord) length.

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  • 2014 · NEET-UG (India) · 4 marks

Two identical long conducting wires AOB and COD are placed at right angle to each other, with one above other such that OO is their common point for the two. The wires carry I1I_1 and I2I_2 currents, respectively. Point PP is lying at distance dd from OO along a direction perpendicular to the plane containing the wires. The magnetic field at the point PP will be:
(a) μ02πd(I1+I2)\frac{\mu_0}{2\pi d}(I_1+I_2) (b) μ02πd(I12−I22)\frac{\mu_0}{2\pi d}(I_1^2-I_2^2) (c) μ02πd(I12+I22)1/2\frac{\mu_0}{2\pi d}(I_1^2+I_2^2)^{1/2} (d) μ02πd(I1I2)\frac{\mu_0}{2\pi d}\left(\frac{I_1}{I_2}\right)

Answer

(c) μ02πd(I12+I22)1/2\frac{\mu_0}{2\pi d}(I_1^2+I_2^2)^{1/2}

Point P is at distance dd from each wire, so each wire gives B=μ0I2πdB=\frac{\mu_0 I}{2\pi d}. The field of each wire at P is perpendicular to the plane containing P and that wire, so the two fields are at right angles to each other. They add as vectors: B=B12+B22=μ02πdI12+I22B=\sqrt{B_1^2+B_2^2}=\frac{\mu_0}{2\pi d}\sqrt{I_1^2+I_2^2}. Simple addition, option (a), ignores the right angle.

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  • 2014 · NEET-UG (India) · 4 marks

In an ammeter 0.2% of main current passes through the galvanometer. If resistance of galvanometer is GG, the resistance of ammeter will be:
(a) 499500G\frac{499}{500}G (b) 1500G\frac{1}{500}G (c) 500499G\frac{500}{499}G (d) 1499G\frac{1}{499}G

Answer

(b) 1500G\frac{1}{500}G

Current through the galvanometer is Ig=I500I_g=\frac{I}{500}, so the shunt carries 499500I\frac{499}{500}I. Equal potential drops give IgG=(I−Ig)SI_gG=(I-I_g)S, so S=G499S=\frac{G}{499}. Ammeter resistance is GG and SS in parallel: RA=GSG+S=G⋅G/499G⋅500/499=G500R_A=\frac{GS}{G+S}=\frac{G\cdot G/499}{G\cdot 500/499}=\frac{G}{500}. Option (d) is only the shunt resistance, not the resistance of the whole ammeter.

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  • 2014 · NEET-UG (India) · 4 marks

Two cities are 150 km apart. Electric power is sent from one city to another city through copper wires. The fall of potential per km is 8 volt and the average resistance per km is 0.5 Ω0.5\ \Omega. The power loss in the wires is:
(a) 19.2 kW (b) 19.2 J (c) 12.2 kW (d) 19.2 W

Answer

(a) 19.2 kW

Total potential fall =8×150=1200=8\times150=1200 V and total resistance =0.5×150=75 Ω=0.5\times150=75\ \Omega. Current I=120075=16I=\frac{1200}{75}=16 A, so power loss =I2R=162×75=19200=I^2R=16^2\times75=19200 W =19.2=19.2 kW. Options (b) and (d) have wrong units: power cannot be in joules, and the value is 19.219.2 kW, not 19.219.2 W.

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  • 2014 · NEET-UG (India) · 4 marks

A potentiometer circuit has been set up for finding the internal resistance of a given cell. The main battery, used across the potentiometer wire, has an emf of 2.0 V and a negligible internal resistance. The potentiometer wire itself is 4 m long. When the resistance RR, connected across the given cell, has values of (i) infinity, (ii) 9.5 Ω9.5\ \Omega, the balancing lengths on the potentiometer wire are found to be 3 m and 2.85 m, respectively. The value of internal resistance of the cell is:
(a) 0.95 Ω0.95\ \Omega (b) 0.5 Ω0.5\ \Omega (c) 0.75 Ω0.75\ \Omega (d) 0.25 Ω0.25\ \Omega

Answer

(b) 0.5 Ω0.5\ \Omega

The balance length for open circuit gives the emf: potential gradient =2.04=0.5=\frac{2.0}{4}=0.5 V/m, so E=0.5×3=1.5E=0.5\times3=1.5 V; with R=9.5 ΩR=9.5\ \Omega, terminal voltage V=0.5×2.85=1.425V=0.5\times2.85=1.425 V. r=R(EV−1)=9.5×(1.51.425−1)=9.5×0.0526=0.5 Ωr=R\left(\frac{E}{V}-1\right)=9.5\times\left(\frac{1.5}{1.425}-1\right)=9.5\times0.0526=0.5\ \Omega. Option (a) results from wrongly using E−V=0.075E-V=0.075 directly with RR.

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  • 2015 · NEET-UG (India) · 4 marks

A proton and an alpha particle both enter a region of uniform magnetic field BB, moving at right angles to the field BB. If the radius of circular orbits for both the particles is equal and the kinetic energy acquired by proton is 1 MeV, the energy acquired by the alpha particle will be:
(a) 1.5 MeV (b) 1 MeV (c) 4 MeV (d) 0.5 MeV

Answer

(b) 1 MeV

Radius r=pqB=2mKqBr=\frac{p}{qB}=\frac{\sqrt{2mK}}{qB}, so for equal rr and BB: K∝q2mK\propto\frac{q^2}{m}. For the alpha particle q=2eq=2e and m=4mpm=4m_p, so q2m=44=1\frac{q^2}{m}=\frac{4}{4}=1 times the proton's value. Hence Kα=1K_\alpha=1 MeV. Option (c) results from forgetting that mass is four times the proton's.

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  • 2015 · NEET-UG (India) · 4 marks

A rectangular coil of length 0.12 m and width 0.1 m having 50 turns of wire is suspended vertically in a uniform magnetic field of strength 0.2 Weber/m2\mathrm{m^2}. The coil carries a current of 2 A. If the plane of the coil is inclined at an angle of 30∘30^\circ with the direction of the field, the torque required to keep the coil in stable equilibrium will be:
(a) 0.24 N m (b) 0.12 N m (c) 0.15 N m (d) 0.20 N m

Answer

(d) 0.20 N m

The magnitude of the torque on a coil is τ=NIABsin⁡θ\tau = NIAB\sin\theta, where θ\theta is the angle between the coil normal and BB. The plane is at 30∘30^\circ to the field, so the normal is at 60∘60^\circ to it. NIAB=50×2×(0.12×0.1)×0.2=0.24NIAB = 50\times2\times(0.12\times0.1)\times0.2 = 0.24 N m, and τ=0.24sin⁡60∘≈0.21≈0.20\tau = 0.24\sin60^\circ \approx 0.21 \approx 0.20 N m. Option (a), 0.24 N m, is only the maximum torque (at θ=90∘\theta=90^\circ), so it is too large.

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  • 2015 · NEET-UG (India) · 4 marks

An electron moves on a straight line path XY. The abcd is a coil adjacent to the path of electron (the circular coil lies in the plane of the path, with a at the top, b on the left, c at the bottom nearest the line, and d on the right; the electron moves from X to Y along the line below the coil). What will be the direction of current, if any, induced in the coil?
(a) The current will reverse its direction as the electron goes past the coil (b) No current induced (c) abcd (d) adcb

Answer

(a) The current will reverse its direction as the electron goes past the coil

As the electron approaches, the magnetic flux through the coil (due to the moving charge) increases, and as it moves away the flux decreases. By Lenz's law the induced current opposes the change, so its sense is one way during approach and the opposite way after the electron has passed. The current is therefore not zero, and it reverses direction; (b) is wrong because the flux changes with time.

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  • 2015 · NEET-UG (India) · 4 marks

A circuit contains an ammeter, a battery of 30 V and a resistance 40.8 ohm all connected in series. If the ammeter has a coil of resistance 480 ohm and a shunt of 20 ohm, the reading in the ammeter will be:
(a) 2 A (b) 1 A (c) 0.5 A (d) 0.25 A

Answer

(c) 0.5 A

The shunt (20 ohm) is in parallel with the coil (480 ohm): RAB=480×20500=19.2 ΩR_{AB}=\dfrac{480\times20}{500}=19.2\ \Omega. Total resistance =40.8+19.2=60 Ω=40.8+19.2=60\ \Omega, so the current in the circuit, which is what the ammeter reads, is I=30/60=0.5I=30/60=0.5 A.

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  • 2016 · NEET-UG (India) · 4 marks

A long solenoid has 1000 turns. When a current of 4 A flows through it, the magnetic flux linked with each turn of the solenoid is 4×10−34\times10^{-3} Wb. The self-inductance of the solenoid is
(a) 1 H (b) 4 H (c) 3 H (d) 2 H

Answer

(a) 1 H

Flux linkage NΦ=LIN\Phi=LI, so L=NΦI=1000×4×10−34=1L=\dfrac{N\Phi}{I}=\dfrac{1000\times4\times10^{-3}}{4}=1 H. Remember the flux given is per turn, so multiply by the number of turns.

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  • 2016 · NEET-UG (India) · 4 marks

A potentiometer wire is 100 cm long and a constant potential difference is maintained across it. Two cells are connected in series first to support one another and then in opposite direction. The balance points are obtained at 50 cm and 10 cm from the positive end of the wire in the two cases. The ratio of emf's is:
(a) 3:23:2 (b) 5:15:1 (c) 5:45:4 (d) 3:43:4

Answer

(a) 3:23:2

Potential gradient is constant, so balance length is proportional to emf. Cells aiding: E1+E2∝50E_1+E_2\propto50. Cells opposing: E1−E2∝10E_1-E_2\propto10. Adding and subtracting: E1∝30E_1\propto30, E2∝20E_2\propto20, so E1:E2=3:2E_1:E_2=3:2.

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  • 2016 · NEET-UG (India) · 4 marks

A long straight wire of radius aa carries a steady current II. The current is uniformly distributed over its cross-section. The ratio of the magnetic fields BB and B′B', at radial distances a2\frac a2 and 2a2a respectively, from the axis of the wire is:
(a) 4 (b) 14\frac14 (c) 12\frac12 (d) 1

Answer

(d) 1

Inside the wire, Ampere's law gives B=μ0Ir2πa2B=\dfrac{\mu_0Ir}{2\pi a^2}, so at r=a2r=\frac a2: B=μ0I4πaB=\dfrac{\mu_0I}{4\pi a}. Outside, B′=μ0I2πrB'=\dfrac{\mu_0I}{2\pi r}, so at r=2ar=2a: B′=μ0I4πaB'=\dfrac{\mu_0I}{4\pi a}. The ratio B/B′=1B/B'=1.

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  • 2016 · NEET-UG (India) · 4 marks

The magnetic susceptibility is negative for:
(a) paramagnetic and ferromagnetic materials (b) diamagnetic material only (c) paramagnetic material only (d) ferromagnetic material only

Answer

(b) diamagnetic material only

Diamagnetic materials get a weak magnetisation opposite to the applied field, so χ\chi is small and negative. Paramagnetic and ferromagnetic materials align with the field, so their χ\chi is positive (small for para, large for ferro).

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  • 2016 · NEET-UG (India) · 4 marks

A square loop ABCD of side LL carrying a current ii is placed near and coplanar with a long straight conductor XY carrying a current II. The side AB of the loop is parallel to the conductor and at a distance L/2L/2 from it, with the loop lying on the side away from the conductor. The net force on the loop will be:
(a) μ0IiL2π\frac{\mu_0 I i L}{2\pi} (b) 2μ0Ii3π\frac{2\mu_0 I i}{3\pi} (c) μ0Ii2π\frac{\mu_0 I i}{2\pi} (d) 2μ0IiL3π\frac{2\mu_0 I i L}{3\pi}

Answer

(b) 2μ0Ii3π\dfrac{2\mu_0Ii}{3\pi}

Forces on the two sides perpendicular to the wire cancel. Side AB (distance L/2L/2) is attracted: F1=μ0Ii L2π(L/2)=μ0IiπF_1=\dfrac{\mu_0Ii\,L}{2\pi(L/2)}=\dfrac{\mu_0Ii}{\pi}. The far side (distance 3L/23L/2) is repelled: F2=μ0Ii L2π(3L/2)=μ0Ii3πF_2=\dfrac{\mu_0Ii\,L}{2\pi(3L/2)}=\dfrac{\mu_0Ii}{3\pi}. Net =F1−F2=2μ0Ii3π=F_1-F_2=\dfrac{2\mu_0Ii}{3\pi}, towards the wire.

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  • 2017 · NEET-UG (India) · 4 marks

The resistance of a wire is RR ohm. If it is melted and stretched to nn times its original length, its new resistance will be
(a) Rn\dfrac{R}{n} (b) n2Rn^2R (c) Rn2\dfrac{R}{n^2} (d) nRnR

Answer

(b) n2Rn^2R

Melting keeps the volume fixed, Al=Al= constant. If l→nll\to nl then A→A/nA\to A/n.

R=ρl/AR=\rho l/A becomes ρ(nl)/(A/n)=n2R\rho(nl)/(A/n)=n^2R.

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  • 2017 · NEET-UG (India) · 4 marks

A 250-turn rectangular coil of length 2.1 cm and width 1.25 cm carries a current of 85 μ85\ \muA and is subjected to a magnetic field of strength 0.85 T. Work done for rotating the coil by 180∘180^\circ against the torque is
(a) 4.55 μ\muJ (b) 2.3 μ\muJ (c) 1.15 μ\muJ (d) 9.1 μ\muJ

Answer

(d) 9.1 μ\muJ

Work done in turning the coil from θ=0\theta=0 to 180∘180^\circ is W=2MB=2NIABW=2MB=2NIAB.

A=2.1×1.25×10−4=2.625×10−4 m2A=2.1\times1.25\times10^{-4}=2.625\times10^{-4}\ \mathrm{m^2}, so W=2×250×85×10−6×2.625×10−4×0.85≈9.5 μW=2\times250\times85\times10^{-6}\times2.625\times10^{-4}\times0.85\approx9.5\ \muJ, which is nearest to 9.1 μ\muJ. The 4.55 μ\muJ option is only MBMB, the work for 90∘90^\circ rotation.

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  • 2017 · NEET-UG (India) · 4 marks

If δ1\delta_1 and δ2\delta_2 be the apparent angles of dip observed in two vertical planes at right angles to each other, then the true angle of dip δ\delta is given by
(a) tan⁡2δ=tan⁡2δ1+tan⁡2δ2\tan^2\delta=\tan^2\delta_1+\tan^2\delta_2 (b) cot⁡2δ=cot⁡2δ1−cot⁡2δ2\cot^2\delta=\cot^2\delta_1-\cot^2\delta_2 (c) tan⁡2δ=tan⁡2δ1−tan⁡2δ2\tan^2\delta=\tan^2\delta_1-\tan^2\delta_2 (d) cot⁡2δ=cot⁡2δ1+cot⁡2δ2\cot^2\delta=\cot^2\delta_1+\cot^2\delta_2

Answer

(d) cot⁡2δ=cot⁡2δ1+cot⁡2δ2\cot^2\delta=\cot^2\delta_1+\cot^2\delta_2

In a vertical plane at angle α\alpha to the meridian, tan⁡δ1=tan⁡δ/cos⁡α\tan\delta_1=\tan\delta/\cos\alpha. For the perpendicular plane, tan⁡δ2=tan⁡δ/sin⁡α\tan\delta_2=\tan\delta/\sin\alpha.

So cot⁡2δ1+cot⁡2δ2=cot⁡2δ(cos⁡2α+sin⁡2α)=cot⁡2δ\cot^2\delta_1+\cot^2\delta_2=\cot^2\delta(\cos^2\alpha+\sin^2\alpha)=\cot^2\delta.

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  • 2017 · NEET-UG (India) · 4 marks

A potentiometer is an accurate and versatile device to make electrical measurements of EMF, because the method involves
(a) potential gradients (b) a condition of no current flow through the galvanometer (c) a combination of cells, galvanometer and resistances (d) cells

Answer

(b) a condition of no current flow through the galvanometer

A potentiometer works on the null (balance) method: at the balance point no current is drawn from the cell being measured, so its EMF is measured without internal-resistance error. Potential gradient is what the wire provides, but the accuracy comes from the zero-current condition.

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  • 2017 · NEET-UG (India) · 4 marks

A long solenoid of diameter 0.1 m has 2×1042\times10^{4} turns per metre. 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 102 π2 Ω10^{2}\ \pi^2\ \Omega, the total charge flowing through the coil during this time is
(a) 16 μ\muC (b) 32 μ\muC (c) 16π\pi μ\muC (d) 32π\pi μ\muC

Answer

(b) 32 μ\muC

Solenoid field B=μ0nIB=\mu_0nI, so ΔΦ=N μ0n ΔI πr2=100×4π×10−7×2×104×4×π×10−4≈3.16×10−3\Delta\Phi=N\,\mu_0 n\,\Delta I\,\pi r^2=100\times4\pi\times10^{-7}\times2\times10^4\times4\times\pi\times10^{-4}\approx3.16\times10^{-3} Wb.

Charge q=ΔΦR=3.16×10−3100π2=32 μq=\dfrac{\Delta\Phi}{R}=\dfrac{3.16\times10^{-3}}{100\pi^2}=32\ \muC. Only the coil area (radius 0.01 m) counts, not the solenoid diameter.

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  • 2018 · NEET-UG (India) · 4 marks

The magnetic potential energy stored in a certain inductor is 25 mJ, when the current in the inductor is 60 mA. This inductor is of inductance
(a) 13.89 H (b) 0.138 H (c) 1.389 H (d) 138.88 H

Answer

(a) 13.89 H

Energy stored in an inductor is U=12LI2U=\tfrac12LI^2.

L=2UI2=2×25×10−3(60×10−3)2=0.053.6×10−3=13.89L=\dfrac{2U}{I^2}=\dfrac{2\times25\times10^{-3}}{(60\times10^{-3})^2}=\dfrac{0.05}{3.6\times10^{-3}}=13.89 H.

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  • 2018 · NEET-UG (India) · 4 marks

A metallic rod of mass per unit length 0.5 kg m−10.5\ \mathrm{kg\,m^{-1}} is lying horizontally on a smooth inclined plane which makes an angle of 30∘30^\circ with the horizontal. The rod is not allowed to slide down by flowing a current through it when a magnetic field of induction 0.25 T is acting on it in the vertical direction. The current flowing in the rod to keep it stationary is
(a) 11.32 A (b) 7.14 A (c) 14.76 A (d) 5.98 A

Answer

(a) 11.32 A

The field is vertical, so the force BIlBIl on the rod is horizontal. Balancing along the smooth incline: BIlcos⁡30∘=mgsin⁡30∘BIl\cos30^\circ = mg\sin30^\circ. I=(m/l) gtan⁡30∘B=0.5×9.8×0.5770.25≈11.32I = \dfrac{(m/l)\,g\tan30^\circ}{B} = \dfrac{0.5 \times 9.8 \times 0.577}{0.25} \approx 11.32 A. Using sin⁡θ\sin\theta instead of tan⁡θ\tan\theta would give a wrong value.

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  • 2018 · NEET-UG (India) · 4 marks

A thin diamagnetic rod is placed vertically between the poles of an electromagnet. When the current in the electromagnet is switched on, the diamagnetic rod is pushed up, out of the horizontal magnetic field. Hence the rod gains gravitational potential energy. The work required to do this comes from
(a) the induced electric field due to the changing magnetic field (b) the current source (c) the lattice structure of the material of the rod (d) the magnetic field

Answer

(b) the current source

Pushing the rod out increases gravitational potential energy, and the magnetic field itself does no work. The changing flux induces an emf in the electromagnet circuit (back emf). The source must supply extra energy to maintain the current against this emf, so the work comes from the current source.

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  • 2018 · NEET-UG (India) · 4 marks

Current sensitivity of a moving coil galvanometer is 5 div/mA and its voltage sensitivity (angular deflection per unit voltage applied) is 20 div/V. The resistance of the galvanometer is
(a) 500 Ω500\ \Omega (b) 40 Ω40\ \Omega (c) 250 Ω250\ \Omega (d) 25 Ω25\ \Omega

Answer

(c) 250 Ω250\ \Omega

Current sensitivity Is=θ/II_s = \theta/I and voltage sensitivity Vs=θ/VV_s = \theta/V, so Vs=Is/RGV_s = I_s/R_G. RG=Is/Vs=5 div/mA20 div/V=0.25 V/mA=250 ΩR_G = I_s/V_s = \dfrac{5\ \text{div/mA}}{20\ \text{div/V}} = 0.25\ \text{V/mA} = 250\ \Omega.

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  • 2018 · NEET-UG (India) · 4 marks

A carbon resistor of (47±4.7) kΩ(47\pm4.7)\ \mathrm{k}\Omega is to be marked with rings of different colours for its identification. The colour code sequence will be
(a) Green - Orange - Violet - Gold (b) Violet - Yellow - Orange - Silver (c) Yellow - Green - Violet - Gold (d) Yellow - Violet - Orange - Silver

Answer

(d) Yellow - Violet - Orange - Silver

47 kΩ=47×10347\ \text{k}\Omega = 47\times10^{3}: first digit 4 = yellow, second digit 7 = violet, multiplier 10310^3 = orange. Tolerance ±10%\pm10\% (4.74.7 kΩ\Omega is 10% of 47 kΩ\Omega) is silver; gold would be 5%.

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  • 2018 · NEET-UG (India) · 4 marks

A set of nn equal resistors, of value RR each, are connected in series to a battery of emf EE and internal resistance RR. The current drawn is II. Now, the nn resistors are connected in parallel to the same battery. Then the current drawn from the battery becomes 10I10I. The value of nn is
(a) 9 (b) 10 (c) 20 (d) 11

Answer

(b) 10

Series: I=EnR+R=E(n+1)RI = \dfrac{E}{nR + R} = \dfrac{E}{(n+1)R}. Parallel: Ip=ER/n+R=nE(n+1)RI_p = \dfrac{E}{R/n + R} = \dfrac{nE}{(n+1)R}. Ip/I=nI_p/I = n, and this is given as 10, so n=10n = 10.

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  • 2019 · NEET-UG (India) · 4 marks

Ionized hydrogen atoms and α\alpha-particles with the same momenta enter perpendicular to a constant magnetic field, BB. The ratio of the radii of their paths rH:rαr_H : r_\alpha will be
(a) 2:12:1 (b) 1:21:2 (c) 4:14:1 (d) 1:41:4

Answer

(a) 2:12:1

Radius r=pqBr = \dfrac{p}{qB}, so for equal momenta r∝1/qr \propto 1/q. qH=eq_H = e, qα=2eq_\alpha = 2e, so rH:rα=2:1r_H : r_\alpha = 2:1. Mass does not matter once momentum is fixed.

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  • 2019 · NEET-UG (India) · 4 marks

In which of the following devices, the eddy current effect is not used?
(a) Induction furnace (b) Magnetic braking in train (c) Electromagnet (d) Electric heater

Answer

(d) Electric heater

Induction furnaces and magnetic braking use eddy currents, and electromagnet cores are laminated precisely to limit them. An electric heater works by Joule heating of a resistive wire carrying a current; it does not use eddy currents.

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  • 2019 · NEET-UG (India) · 4 marks

Which of the following acts as a circuit protection device?
(a) Conductor (b) Inductor (c) Switch (d) Fuse

Answer

(d) Fuse

A fuse has a thin wire that melts when current exceeds a safe limit, breaking the circuit and protecting it. A conductor only carries current, an inductor opposes current changes, and a switch is operated by hand, so none of these protects automatically.

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  • 2019 · NEET-UG (India) · 4 marks

At a point AA on the earth's surface the angle of dip, δ=+25∘\delta=+25^\circ. At a point BB on the earth's surface the angle of dip, δ=−25∘\delta=-25^\circ. We can interpret that
(a) AA and BB are both located in the northern hemisphere. (b) AA is located in the southern hemisphere and BB is located in the northern hemisphere. (c) AA is located in the northern hemisphere and BB is located in the southern hemisphere. (d) AA and BB are both located in the southern hemisphere.

Answer

(c) AA is located in the northern hemisphere and BB is located in the southern hemisphere.

By convention, the dip angle is positive when the north pole of the needle dips below the horizontal, which happens in the northern hemisphere. It is negative in the southern hemisphere, where the south end dips. So +25∘+25^\circ is north and −25∘-25^\circ is south.

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  • 2019 · NEET-UG (India) · 4 marks

A 800 turn coil of effective area 0.05 m20.05\ \mathrm{m^2} is kept perpendicular to a magnetic field 5×10−55\times10^{-5} T. When the plane of the coil is rotated by 90∘90^\circ around any of its coplanar axis in 0.1 s, the emf induced in the coil will be
(a) 2 V (b) 0.2 V (c) 2×10−32\times10^{-3} V (d) 0.02 V

Answer

(d) 0.02 V

Initial flux =NBA=NBA (coil perpendicular to field), final flux =0=0 after a 90∘90^\circ turn. ε=NBAt=800×5×10−5×0.050.1=0.02\varepsilon=\dfrac{NBA}{t}=\dfrac{800\times5\times10^{-5}\times0.05}{0.1}=0.02 V.

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  • 2020 · NEET-UG (India) · 4 marks

The solids which have the negative temperature coefficient of resistance are
(a) semiconductors only (b) insulators and semiconductors (c) metals (d) insulators only

Answer

(b) insulators and semiconductors

In insulators and semiconductors, heating frees more charge carriers, so resistance falls as temperature rises (negative α\alpha). In metals, more lattice vibration increases collisions, so resistance rises (positive α\alpha).

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  • 2020 · NEET-UG (India) · 4 marks

A long solenoid of 50 cm length having 100 turns carries a current 2.5 A. The magnetic field at the centre of the solenoid is (μ0=4π×10−7 T m A−1\mu_0=4\pi\times10^{-7}\ \mathrm{T\,m\,A^{-1}})
(a) 6.28×10−56.28\times10^{-5} T (b) 3.14×10−53.14\times10^{-5} T (c) 6.28×10−46.28\times10^{-4} T (d) 3.14×10−43.14\times10^{-4} T

Answer

(c) 6.28×10−46.28\times10^{-4} T

B=μ0nIB=\mu_0nI with n=1000.5=200n=\dfrac{100}{0.5}=200 turns/m. B=4π×10−7×200×2.5=6.28×10−4B=4\pi\times10^{-7}\times200\times2.5=6.28\times10^{-4} T. Using 0.5 m wrongly as the turns-per-length would give the smaller options.

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  • 2020 · NEET-UG (India) · 4 marks

An iron rod of susceptibility 599 is subjected to a magnetising field of 1200 A m−11200\ \mathrm{A\,m^{-1}}. The permeability of the material of the rod is: (μ0=4π×10−7 T m A−1\mu_0=4\pi\times10^{-7}\ \mathrm{T\,m\,A^{-1}})
(a) 2.4π×10−5 T m A−12.4\pi\times10^{-5}\ \mathrm{T\,m\,A^{-1}} (b) 2.4π×10−7 T m A−12.4\pi\times10^{-7}\ \mathrm{T\,m\,A^{-1}} (c) 2.4π×10−4 T m A−12.4\pi\times10^{-4}\ \mathrm{T\,m\,A^{-1}} (d) 8.0×10−5 T m A−18.0\times10^{-5}\ \mathrm{T\,m\,A^{-1}}

Answer

(c) 2.4π×10−4 T m A−12.4\pi\times10^{-4}\ \mathrm{T\,m\,A^{-1}}

μ=μ0(1+χ)=4π×10−7×600=2.4π×10−4\mu=\mu_0(1+\chi)=4\pi\times10^{-7}\times600=2.4\pi\times10^{-4} T m A−1^{-1}. The field HH is not needed for μ\mu; forgetting the 11 in 1+χ1+\chi gives a slightly different, wrong value.

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  • 2020 · NEET-UG (India) · 4 marks

A resistance wire connected in the left gap of a metre bridge balances a 10 Ω10\ \Omega resistance in the right gap at a point which divides the bridge wire in the ratio 3:23:2. If the length of the resistance wire is 1.5 m, then the length of 1 Ω1\ \Omega of the resistance wire is
(a) 1.5×10−11.5\times10^{-1} m (b) 1.5×10−21.5\times10^{-2} m (c) 1.0×10−21.0\times10^{-2} m (d) 1.0×10−11.0\times10^{-1} m

Answer

(d) 1.0×10−11.0\times10^{-1} m

At balance, X10=l100−l=32\dfrac{X}{10}=\dfrac{l}{100-l}=\dfrac32, so X=15 ΩX=15\ \Omega. This wire of 1.5 m has 15 Ω\Omega, so 1 Ω\Omega corresponds to 1.5/15=0.11.5/15=0.1 m.

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  • 2020 · NEET-UG (India) · 4 marks

A charged particle having drift velocity of 7.5×10−4 m s−17.5\times10^{-4}\ \mathrm{m\,s^{-1}} in an electric field of 3×10−10 V m−13\times10^{-10}\ \mathrm{V\,m^{-1}} has a mobility in m2 V−1 s−1\mathrm{m^2\,V^{-1}\,s^{-1}} of
(a) 2.5×10−62.5\times10^{-6} (b) 2.25×10−152.25\times10^{-15} (c) 2.25×10152.25\times10^{15} (d) 2.5×1062.5\times10^{6}

Answer

(d) 2.5×1062.5\times10^{6}

Mobility μ=vdE=7.5×10−43×10−10=2.5×106 m2 V−1 s−1\mu=\dfrac{v_d}{E}=\dfrac{7.5\times10^{-4}}{3\times10^{-10}}=2.5\times10^{6}\ \mathrm{m^2\,V^{-1}\,s^{-1}}. The exponent is −4−(−10)=+6-4-(-10)=+6, so the negative-exponent options are wrong.

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  • 2021 · NEET-UG (India) · 4 marks

The effective resistance of a parallel connection that consists of four wires of equal length, equal area of cross-section and same material is 0.25 Ω0.25\ \Omega. What will be the effective resistance if they are connected in series?
(a) 1 Ω1\ \Omega (b) 4 Ω4\ \Omega (c) 0.25 Ω0.25\ \Omega (d) 0.5 Ω0.5\ \Omega

Answer

(b) 4 Ω4\ \Omega

Four identical wires of resistance RR in parallel give R/4=0.25 ΩR/4=0.25\ \Omega, so R=1 ΩR=1\ \Omega. In series they give 4R=4 Ω4R=4\ \Omega. The tempting 1 Ω1\ \Omega is the resistance of a single wire, not of the series combination.

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  • 2021 · NEET-UG (India) · 4 marks

Column-I gives certain physical terms associated with flow of current through a metallic conductor. Column-II gives some mathematical relations involving electrical quantities. Match Column-I and Column-II with appropriate relations.
Column-I: (A) Drift velocity; (B) Electrical resistivity; (C) Relaxation period; (D) Current density
Column-II: (P) mne2ρ\frac{m}{ne^2\rho}; (Q) nevdnev_d; (R) eEτm\frac{eE\tau}{m}; (S) EJ\frac{E}{J}
(a) A-R, B-P, C-S, D-Q (b) A-R, B-Q, C-S, D-P (c) A-R, B-S, C-P, D-Q (d) A-R, B-S, C-Q, D-P

Answer

(c) A-R, B-S, C-P, D-Q

Drift velocity vd=eEτmv_d=\frac{eE\tau}{m} (R); resistivity ρ=EJ\rho=\frac{E}{J} (S); from ρ=mne2τ\rho=\frac{m}{ne^2\tau} the relaxation time is τ=mne2ρ\tau=\frac{m}{ne^2\rho} (P); current density J=nevdJ=nev_d (Q). The other options swap resistivity and relaxation period.

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  • 2021 · NEET-UG (India) · 4 marks

In a potentiometer circuit a cell of EMF 1.5 V gives balance point at 36 cm length of wire. If another cell of EMF 2.5 V replaces the first cell, then at what length of the wire, the balance point occurs?
(a) 64 cm (b) 62 cm (c) 60 cm (d) 21.6 cm

Answer

(c) 60 cm

In a potentiometer, balance length is proportional to EMF. l2l1=E2E1\frac{l_2}{l_1}=\frac{E_2}{E_1}, so l2=36×2.51.5=60l_2=36\times\frac{2.5}{1.5}=60 cm. The value 21.6 cm comes from wrongly multiplying by the inverse ratio.

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  • 2021 · NEET-UG (India) · 4 marks

An infinitely long straight conductor carries a current of 5 A. An electron is moving with a speed of 10510^5 m/s parallel to the conductor. The perpendicular distance between the electron and the conductor is 20 cm at an instant. Calculate the magnitude of the force experienced by the electron at the instant.
(a) 4π×10−204\pi \times 10^{-20} N (b) 8×10−208 \times 10^{-20} N (c) 4×10−204 \times 10^{-20} N (d) 8π×10−208\pi \times 10^{-20} N

Answer

(b) 8×10−208\times10^{-20} N

Field of the wire at 20 cm: B=μ0I2πr=2×10−7×50.2=5×10−6B=\frac{\mu_0 I}{2\pi r}=\frac{2\times10^{-7}\times5}{0.2}=5\times10^{-6} T. The electron's velocity is parallel to the wire, hence perpendicular to BB, so F=evB=1.6×10−19×105×5×10−6=8×10−20F=evB=1.6\times10^{-19}\times10^5\times5\times10^{-6}=8\times10^{-20} N.

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  • 2021 · NEET-UG (India) · 4 marks

Two conducting circular loops of radii R1R_1 and R2R_2 are placed in the same plane with their centres coinciding. If R1≫R2R_1 \gg R_2, the mutual inductance MM between them will be directly proportional to:
(a) R12R2\frac{R_1^2}{R_2} (b) R22R1\frac{R_2^2}{R_1} (c) R1R2\frac{R_1}{R_2} (d) R2R1\frac{R_2}{R_1}

Answer

(b) R22R1\frac{R_2^2}{R_1}

Take current II in the large loop. The field at the centre is B=μ0I2R1B=\frac{\mu_0I}{2R_1}, nearly uniform over the small loop. Flux =BπR22=μ0πIR222R1=B\pi R_2^2=\frac{\mu_0\pi IR_2^2}{2R_1}, so M∝R22R1M\propto\frac{R_2^2}{R_1}.

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  • 2021 · NEET-UG (India) · 4 marks

In the product F⃗=q(v⃗×B⃗)=qv⃗×(Bi^+Bj^+B0k^)\vec{F} = q(\vec{v} \times \vec{B}) = q\vec{v} \times (B\hat{i} + B\hat{j} + B_0\hat{k}), for q=1q = 1 and v⃗=2i^+4j^+6k^\vec{v} = 2\hat{i} + 4\hat{j} + 6\hat{k} and F⃗=4i^−20j^+12k^\vec{F} = 4\hat{i} - 20\hat{j} + 12\hat{k}, what will be the complete expression for B⃗\vec{B}?
(a) 8i^+8j^−6k^8\hat{i} + 8\hat{j} - 6\hat{k} (b) 6i^+6j^−8k^6\hat{i} + 6\hat{j} - 8\hat{k} (c) −8i^−8j^−6k^-8\hat{i} - 8\hat{j} - 6\hat{k} (d) −6i^−6j^−8k^-6\hat{i} - 6\hat{j} - 8\hat{k}

Answer

(d) −6i^−6j^−8k^-6\hat i-6\hat j-8\hat k

With B⃗=(B,B,B0)\vec B=(B,B,B_0) and v⃗=(2,4,6)\vec v=(2,4,6): v⃗×B⃗=(4B0−6B, 6B−2B0, 2B−4B)\vec v\times\vec B=(4B_0-6B,\ 6B-2B_0,\ 2B-4B). The k^\hat k term gives −2B=12-2B=12, so B=−6B=-6. The j^\hat j term gives −36−2B0=−20-36-2B_0=-20, so B0=−8B_0=-8. Check the i^\hat i term: −32+36=4-32+36=4. Hence B⃗=−6i^−6j^−8k^\vec B=-6\hat i-6\hat j-8\hat k.

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  • 2022 · NEET-UG (India) · 4 marks

As the temperature increases, the electrical resistance:
(a) Increases for both conductors and semiconductors (b) Decreases for both conductors and semiconductors (c) Increases for conductors but decreases for semiconductors (d) Decreases for conductors but increases for semiconductors

Answer

(c) Increases for conductors but decreases for semiconductors

In conductors, collisions increase with temperature, so resistance rises (positive temperature coefficient). In semiconductors, heating frees more charge carriers, which outweighs increased collisions, so resistance falls (negative temperature coefficient).

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  • 2022 · NEET-UG (India) · 4 marks

A long solenoid of radius 1 mm has 100 turns per mm. If 1 A current flows in the solenoid, the magnetic field strength at the centre of the solenoid is:
(a) 6.28×10−26.28 \times 10^{-2} T (b) 12.56×10−212.56 \times 10^{-2} T (c) 12.26×10−412.26 \times 10^{-4} T (d) 6.28×10−46.28 \times 10^{-4} T

Answer

(b) 12.56×10−212.56 \times 10^{-2} T

Inside a long solenoid B=μ0nIB = \mu_0 n I. Here n=100n = 100 turns/mm =105= 10^5 turns/m, so B=4π×10−7×105×1=0.1256B = 4\pi\times10^{-7}\times10^{5}\times1 = 0.1256 T =12.56×10−2= 12.56\times10^{-2} T. The radius of 1 mm is not needed.

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  • 2022 · NEET-UG (India) · 4 marks

A copper wire of length 10 m and radius (10−2π)\left(\frac{10^{-2}}{\sqrt{\pi}}\right) m has electrical resistance of 10 Ω\Omega. The current density in the wire for an electric field strength of 10 (V/m) is:
(a) 104 A/m210^4\ \mathrm{A/m^2} (b) 106 A/m210^6\ \mathrm{A/m^2} (c) 10−5 A/m210^{-5}\ \mathrm{A/m^2} (d) 105 A/m210^5\ \mathrm{A/m^2}

Answer

(d) 105 A/m210^5\ \mathrm{A/m^2}

Area A=πr2=10−4 m2A = \pi r^2 = 10^{-4}\ \mathrm{m^2}. Resistivity ρ=RA/L=10×10−4/10=10−4 Ω \rho = RA/L = 10\times10^{-4}/10 = 10^{-4}\ \Omega\,m. Current density J=E/ρ=10/10−4=105 A/m2J = E/\rho = 10/10^{-4} = 10^5\ \mathrm{A/m^2}.

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  • 2022 · NEET-UG (India) · 4 marks

A square loop of side 1 m and resistance 1 Ω\Omega is placed in a magnetic field of 0.5 T. If the plane of loop is perpendicular to the direction of magnetic field, the magnetic flux through the loop is:
(a) 2 weber (b) 0.5 weber (c) 1 weber (d) Zero weber

Answer

(b) 0.5 weber

Flux ϕ=BAcos⁡θ\phi = BA\cos\theta with the plane perpendicular to the field, so the normal is parallel to BB and θ=0\theta=0. ϕ=0.5×(1×1)=0.5\phi = 0.5\times(1\times1) = 0.5 Wb. The resistance is irrelevant here.

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  • 2022 · NEET-UG (India) · 4 marks

Given below are two statements.
Statement I: Biot-Savart's law gives an expression for the magnetic field strength of an infinitesimal current element (IdlIdl) of a current carrying conductor only.
Statement II: Biot-Savart's law is analogous to Coulomb's inverse square law of charge qq, with the former being related to the field produced by a scalar source, IdlIdl, while the latter being produced by a vector source, qq.
In light of above statements choose the most appropriate answer from the options given below:
(a) Both Statement I and Statement II are correct (b) Both Statement I and Statement II are incorrect (c) Statement I is correct and Statement II is incorrect (d) Statement I is incorrect and Statement II is correct

Answer

(c) Statement I is correct and Statement II is incorrect

Biot-Savart law gives the field of a current element IdlIdl only, so Statement I is correct. In Statement II the roles are reversed: IdlIdl is a vector source while the charge qq is a scalar source, so the statement is wrong.

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  • 2022 · NEET-UG (India) · 4 marks

Two resistors of resistances 100 Ω\Omega and 200 Ω\Omega are connected in parallel in an electrical circuit. The ratio of thermal energy developed in 100 Ω\Omega to that in 200 Ω\Omega in a given time is:
(a) 1 : 2 (b) 2 : 1 (c) 1 : 4 (d) 4 : 1

Answer

(b) 2 : 1

In parallel the voltage is the same, so H=V2t/R∝1/RH = V^2t/R\propto 1/R. Hence H100:H200=200:100=2:1H_{100}:H_{200} = 200:100 = 2:1. Using I2RI^2R with the same current is wrong because the currents differ.

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  • 2022 · NEET-UG (India) · 4 marks

From Ampere's circuital law for a long straight wire of circular cross-section carrying a steady current, the variation of magnetic field in the inside and outside region of the wire is:
(a) Uniform and remains constant for both the regions (b) A linearly increasing function of distance up to the boundary of the wire and then linearly decreasing for the outside region (c) A linearly increasing function of distance rr up to the boundary of the wire and then decreasing one with 1/r1/r dependence for the outside region (d) A linearly decreasing function of distance up to the boundary of the wire and then a linearly increasing one for the outside region

Answer

(c) A linearly increasing function of distance rr up to the boundary of the wire and then decreasing one with 1/r1/r dependence for the outside region

Inside, the enclosed current is Ir2/a2I r^2/a^2, so B=μ0Ir2πa2∝rB = \dfrac{\mu_0 I r}{2\pi a^2}\propto r. Outside, the full current is enclosed, so B=μ0I2πr∝1/rB=\dfrac{\mu_0 I}{2\pi r}\propto 1/r.

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  • 2022 · NEET-UG (India) · 4 marks

A big circular coil of 1000 turns and average radius 10 m is rotating about its horizontal diameter at 2 rad s−12\ \mathrm{rad\,s^{-1}}. If the vertical component of earth's magnetic field at that place is 2×10−52 \times 10^{-5} T and electrical resistance of the coil is 12.56 Ω12.56\ \Omega, then the maximum induced current in the coil will be:
(a) 0.25 A (b) 1.5 A (c) 1 A (d) 2 A

Answer

(c) 1 A

Maximum emf =NBAω=1000×2×10−5×π(10)2×2=12.56= NBA\omega = 1000\times2\times10^{-5}\times\pi(10)^2\times2 = 12.56 V. Maximum current =12.56/12.56=1= 12.56/12.56 = 1 A.

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  • 2023 · NEET-UG (India) · 4 marks

The magnetic energy stored in an inductor of inductance 4 H carrying a current of 2 A is:
(a) 4 J (b) 4 mJ (c) 8 mJ (d) 8 J

Answer

(d) 8 J

U=12LI2=12×4×22=8U = \tfrac12LI^2 = \tfrac12\times4\times2^2 = 8 J.

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  • 2023 · NEET-UG (India) · 4 marks

Resistance of a carbon resistor determined from colour codes is (22000±5%) Ω(22000 \pm 5\%)\ \Omega. The colour of third band must be:
(a) Red (b) Green (c) Orange (d) Yellow

Answer

(c) Orange

22000 Ω=22×103 Ω22000\ \Omega = 22\times10^{3}\ \Omega. The first two bands give 2 and 2 (red, red), and the third band is the multiplier 10310^3, which is orange. Yellow would be 10410^4 and green 10510^5.

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  • 2023 · NEET-UG (India) · 4 marks

The net magnetic flux through any closed surface is:
(a) Zero (b) Positive (c) Infinity (d) Negative

Answer

(a) Zero

Magnetic monopoles do not exist, so field lines form closed loops: as many lines enter a closed surface as leave it. Hence ∮B⃗⋅dA⃗=0\oint\vec B\cdot d\vec A=0 (Gauss's law for magnetism).

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  • 2023 · NEET-UG (India) · 4 marks

10 resistors, each of resistance RR are connected in series to a battery of emf EE and negligible internal resistance. Then those are connected in parallel to the same battery, the current is increased nn times. The value of nn is:
(a) 10 (b) 100 (c) 1 (d) 1000

Answer

(b) 100

Series: Rs=10RR_s=10R, so Is=E10RI_s=\frac{E}{10R}. Parallel: Rp=R10R_p=\frac{R}{10}, so Ip=10ERI_p=\frac{10E}{R}. Ratio n=IpIs=100n=\frac{I_p}{I_s}=100.

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  • 2023 · NEET-UG (India) · 4 marks

The resistance of platinum wire at 0∘0^\circC is 2 Ω2\ \Omega and 6.8 Ω6.8\ \Omega at 80∘80^\circC. The temperature coefficient of resistance of the wire is:
(a) 3×10−4 ∘C−13 \times 10^{-4}\ ^\circ\mathrm{C}^{-1} (b) 3×10−3 ∘C−13 \times 10^{-3}\ ^\circ\mathrm{C}^{-1} (c) 3×10−2 ∘C−13 \times 10^{-2}\ ^\circ\mathrm{C}^{-1} (d) 3×10−1 ∘C−13 \times 10^{-1}\ ^\circ\mathrm{C}^{-1}

Answer

(c) 3×10−2 ∘C−13\times10^{-2}\ ^\circ\mathrm{C}^{-1}

Rt=R0(1+αt)R_t=R_0(1+\alpha t) gives α=Rt−R0R0t=6.8−22×80=4.8160=3×10−2 ∘C−1\alpha=\frac{R_t-R_0}{R_0t}=\frac{6.8-2}{2\times80}=\frac{4.8}{160}=3\times10^{-2}\ ^\circ\mathrm{C}^{-1}.

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  • 2023 · NEET-UG (India) · 4 marks

A wire carrying a current II along the positive xx-axis has length LL. It is kept in a magnetic field B⃗=(2i^+3j^−4k^)\vec{B} = (2\hat{i} + 3\hat{j} - 4\hat{k}) T. The magnitude of the magnetic force acting on the wire is:
(a) 3IL3IL (b) 5 IL\sqrt{5}\,IL (c) 5IL5IL (d) 3 IL\sqrt{3}\,IL

Answer

(c) 5IL5IL

F⃗=IL⃗×B⃗=IL i^×(2i^+3j^−4k^)=IL(3k^+4j^)\vec F=I\vec L\times\vec B = IL\,\hat i\times(2\hat i+3\hat j-4\hat k)=IL(3\hat k+4\hat j). Magnitude =IL9+16=5IL=IL\sqrt{9+16}=5IL. The xx-component of B⃗\vec B is parallel to the wire and gives no force.

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  • 2024 · NEET-UG (India) · 4 marks

Match List - I with List - II.
List - I (Material): A. Diamagnetic; B. Ferromagnetic; C. Paramagnetic; D. Non-magnetic
List - II (Susceptibility χ\chi): I. χ=0\chi = 0; II. 0>χ≥−10 > \chi \ge -1; III. χ≫1\chi \gg 1; IV. 0<χ<ε0 < \chi < \varepsilon (ε\varepsilon a small positive number)
Choose the correct answer from the options given below:
(a) A-II, B-I, C-III, D-IV (b) A-III, B-II, C-I, D-IV (c) A-IV, B-III, C-II, D-I (d) A-II, B-III, C-IV, D-I

Answer

(d) A-II, B-III, C-IV, D-I

Diamagnetic: small negative χ\chi (0>χ≥−10>\chi\ge-1). Ferromagnetic: χ≫1\chi\gg1. Paramagnetic: small positive χ\chi. Non-magnetic: χ=0\chi=0.

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  • 2024 · NEET-UG (India) · 4 marks

A tightly wound 100 turns coil of radius 10 cm carries a current of 7 A. The magnitude of the magnetic field at the centre of the coil is (Take permeability of free space as 4π×10−74\pi \times 10^{-7} SI units):
(a) 4.4 T (b) 4.4 mT (c) 44 T (d) 44 mT

Answer

(b) 4.4 mT

B=μ0NI2R=4π×10−7×100×72×0.1=4.4×10−3B=\frac{\mu_0NI}{2R}=\frac{4\pi\times10^{-7}\times100\times7}{2\times0.1}=4.4\times10^{-3} T =4.4=4.4 mT.

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  • 2024 · NEET-UG (India) · 4 marks

The terminal voltage of the battery, whose emf is 10 V and internal resistance 1 Ω1\ \Omega, when connected through an external resistance of 4 Ω4\ \Omega is:
(a) 6 V (b) 8 V (c) 10 V (d) 4 V

Answer

(b) 8 V

Current I=ER+r=104+1=2I=\frac{E}{R+r}=\frac{10}{4+1}=2 A. Terminal voltage V=E−Ir=10−2=8V=E-Ir=10-2=8 V (equivalently IR=2×4IR=2\times4).

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  • 2024 · NEET-UG (India) · 4 marks

A wire of length ll and resistance 100 Ω100\ \Omega is divided into 10 equal parts. The first 5 parts are connected in series while the next 5 parts are connected in parallel. The two combinations are again connected in series. The resistance of this final combination is:
(a) 52 Ω52\ \Omega (b) 55 Ω55\ \Omega (c) 60 Ω60\ \Omega (d) 26 Ω26\ \Omega

Answer

(a) 52 Ω52\ \Omega

Each part is 10 Ω10\ \Omega. Five in series give 50 Ω50\ \Omega; five in parallel give 105=2 Ω\frac{10}{5}=2\ \Omega. Total in series: 50+2=52 Ω50+2=52\ \Omega.

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  • 2024 · NEET-UG (India) · 4 marks

In a uniform magnetic field of 0.049 T, a magnetic needle performs 20 complete oscillations in 5 seconds. The moment of inertia of the needle is 9.8×10−6 kg m29.8 \times 10^{-6}\ \mathrm{kg\,m^2}. If the magnitude of the magnetic moment of the needle is x×10−5 A m2x \times 10^{-5}\ \mathrm{A\,m^2}, then the value of xx is:
(a) 128π2128\pi^2 (b) 50π250\pi^2 (c) 1280π21280\pi^2 (d) 5π25\pi^2

Answer

(c) 1280π21280\pi^2

Period T=520=0.25T=\frac{5}{20}=0.25 s. For a magnetic needle T=2πIMBT=2\pi\sqrt{\frac{I}{MB}}, so M=4π2IBT2M=\frac{4\pi^2 I}{BT^2}. M=4π2(9.8×10−6)0.049×0.0625=4π2×3.2×10−3=1.28×10−2π2=1280π2×10−5 A m2M=\frac{4\pi^2(9.8\times10^{-6})}{0.049\times0.0625}=4\pi^2\times3.2\times10^{-3}=1.28\times10^{-2}\pi^2=1280\pi^2\times10^{-5}\ \mathrm{A\,m^2}. So x=1280π2x=1280\pi^2. A common slip is using the frequency in place of the period.

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  • 2024 · NEET-UG (India) · 4 marks

Two heaters A and B have power rating of 1 kW and 2 kW, respectively. Those two are first connected in series and then in parallel to a fixed power source. The ratio of power outputs for these two cases is:
(a) 2 : 9 (b) 1 : 2 (c) 2 : 3 (d) 1 : 1

Answer

(a) 2 : 9

With supply voltage VV, RA=V21000R_A=\frac{V^2}{1000} and RB=V22000R_B=\frac{V^2}{2000}. Series: Ps=V2RA+RB=V23V2/2000=20003P_s=\frac{V^2}{R_A+R_B}=\frac{V^2}{3V^2/2000}=\frac{2000}{3} W. Parallel: Pp=1000+2000=3000P_p=1000+2000=3000 W. Ratio Ps:Pp=20003:3000=2:9P_s:P_p=\frac{2000}{3}:3000=2:9.

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  • 2024 · NEET-UG (India) · 4 marks

A sheet is placed on a horizontal surface in front of a strong magnetic pole. A force is needed to:
A. hold the sheet there if it is magnetic B. hold the sheet there if it is non-magnetic. C. move the sheet away from the pole with uniform velocity if it is conducting. D. move the sheet away from the pole with uniform velocity if it is both, non-conducting and non-polar.
Choose the correct statement(s) from the options given below:
(a) A and C only (b) A, C and D only (c) C only (d) B and D only

Answer

(a) A and C only

A: a magnetic sheet is attracted by the strong pole, so a force is needed to hold it in place. C: moving a conductor away from the pole changes the flux through it, so eddy currents arise and (Lenz's law) oppose the motion, and a force is needed even at uniform velocity. B is wrong because a non-magnetic sheet feels no static force. D is wrong because a non-conducting, non-polar sheet has neither magnetic attraction nor eddy currents.

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  • 2025 · NEET-UG (India) · 4 marks

A wire of resistance RR is cut into 8 equal pieces. From these pieces two equivalent resistances are made by adding four of these together in parallel. Then these two sets are added in series. The net effective resistance of the combination is:
(a) R16\frac{R}{16} (b) R8\frac{R}{8} (c) R64\frac{R}{64} (d) R32\frac{R}{32}

Answer

(a) R16\frac{R}{16}

Each of the 8 pieces has resistance R8\frac R8. Four in parallel: R/84=R32\frac{R/8}{4}=\frac{R}{32}. Two such sets in series: R32+R32=R16\frac{R}{32}+\frac{R}{32}=\frac{R}{16}.

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  • 2025 · NEET-UG (India) · 4 marks

An electron (mass 9×10−319 \times 10^{-31} kg and charge 1.6×10−191.6 \times 10^{-19} C) moving with speed c/100c/100 (cc = speed of light) is injected into a magnetic field BB of magnitude 9×10−49 \times 10^{-4} T perpendicular to its direction of motion. We wish to apply a uniform electric field EE together with the magnetic field so that the electron does not deflect from its path. Then (speed of light c=3×108 m s−1c = 3 \times 10^{8}\ \mathrm{m\,s^{-1}}):
(a) EE is parallel to BB and its magnitude is 27×102 V m−127 \times 10^{2}\ \mathrm{V\,m^{-1}} (b) EE is parallel to BB and its magnitude is 27×104 V m−127 \times 10^{4}\ \mathrm{V\,m^{-1}} (c) EE is perpendicular to BB and its magnitude is 27×104 V m−127 \times 10^{4}\ \mathrm{V\,m^{-1}} (d) EE is perpendicular to BB and its magnitude is 27×102 V m−127 \times 10^{2}\ \mathrm{V\,m^{-1}}

Answer

(d) EE is perpendicular to BB and its magnitude is 27×102 V m−127\times10^{2}\ \mathrm{V\,m^{-1}}

For no deflection the electric and magnetic forces balance: eE=evBeE=evB, so E=vBE=vB. The magnetic force is perpendicular to both vv and BB, so EE must also be perpendicular to BB (and to vv); a field parallel to BB cannot cancel it. v=c100=3×106v=\frac{c}{100}=3\times10^6 m/s, so E=3×106×9×10−4=2.7×103=27×102E=3\times10^6\times9\times10^{-4}=2.7\times10^3=27\times10^2 V/m.

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  • 2025 · NEET-UG (India) · 4 marks

A 2 A current is flowing through two different small circular copper coils having radii ratio 1 : 2. The ratio of their respective magnetic moments will be:
(a) 2 : 1 (b) 4 : 1 (c) 1 : 4 (d) 1 : 2

Answer

(c) 1 : 4

Magnetic moment of a single-turn coil is M=IA=Iπr2M=IA=I\pi r^2. The current is the same (2 A), so M∝r2M\propto r^2. M1M2=(12)2=14\frac{M_1}{M_2}=\left(\frac12\right)^2=\frac14, i.e. 1 : 4.

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Questions from NEET-UG 2013 (India), Code W (NTA NEET-UG 2013 question paper; only questions on topics in Nepal's MBBS entrance syllabus), AIPMT 2014 (India), main paper (NTA NEET-UG 2014 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2015 (India), Code C (re-exam) (NTA NEET-UG 2015 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2016 (India), Phase 1 Code C/R/Y (NTA NEET-UG 2016 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2017 (India), Code B (NTA NEET-UG 2017 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2018 (India), Code NN (NTA NEET-UG 2018 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2019 (India), Code P1 (NTA NEET-UG 2019 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2020 (India), Code F1 (13 September 2020) (NTA NEET-UG 2020 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2021 (India), Paper Code O1 (12 September 2021) (NTA NEET-UG 2021 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2022 (India), Paper Code Q6 (17 July 2022) (NTA NEET-UG 2022 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2023 (India), 7 May 2023 (NTA NEET-UG 2023 question paper; only questions on topics in Nepal's MBBS entrance syllabus), NEET-UG 2024 (India), Paper Code R3 (5 May 2024) (NTA NEET-UG 2024 question paper; only questions on topics in Nepal's MBBS entrance syllabus) and NEET-UG 2025 (India), Paper Code Narmada 48 (4 May 2025) (NTA NEET-UG 2025 question paper; only questions on topics in Nepal's MBBS entrance syllabus). Answers are written for this site; check them against your class notes.