33 Years NEET-AIPMT Chapterwise Solutions - Physics 2020

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Magnetism and MatterTelegram @unacademyplusdiscounts53Which one of the following is true?(a) B is of a paramagnetic material(b) C is of a diamagnetic material(c) D is of a ferromagnetic material(d) A is of a non-magnetic material (2011)25. The magnetic moment of a diamagnetic atom is(a) much greater than one(b) 1(c) between zero and one(d) equal to zero (Mains 2010)26. If a diamagnetic substance is brought near the northor the south pole of a bar magnet, it is(a) repelled by the north pole and attracted by thesouth pole(b) attracted by the north pole and repelled by thesouth pole(c) attracted by both the poles(d) repelled by both the poles (2009, 1999)27. Curie temperature above which(a) paramagnetic material becomes ferromagneticmaterial(b) ferromagnetic material becomes diamagneticmaterial(c) ferromagnetic material becomes paramagneticmaterial(d) paramagnetic material becomes diamagneticmaterial (2008, 2006)28. Nickel shows ferromagnetic property at roomtemperature. If the temperature is increased beyondCurie temperature, then it will show(a) anti ferromagnetism(b) no magnetic property(c) diamagnetism(d) paramagnetism. (2007)29. If the magnetic dipole moment of an atom ofdiamagnetic material, paramagnetic material andferromagnetic material are denoted by m d , m p and m frespectively, then(a) m d = 0 and m p ≠ 0 (b) m d ≠ 0 and m p = 0(c) m p = 0 and m f ≠ 0 (d) m d ≠ 0 and m f ≠ 0.(2005)30. A diamagnetic material in a magnetic field moves(a) from stronger to the weaker parts of the field(b) from weaker to the stronger parts of the field(c) perpendicular to the field(d) in none of the above directions (2003)31. According to Curie’s law, the magnetic susceptibilityof a substance at an absolute temperature T isproportional to(a) 1/T(b) T(c) 1/T 2 (d) T 2 (2003)32. Among which the magnetic susceptibility does notdepend on the temperature?(a) Diamagnetism (b) Paramagnetism(c) Ferromagnetism (d) Ferrite. (2001)33. For protecting a sensitive equipment from theexternal magnetic field, it should be(a) surrounded with fine copper sheet(b) placed inside an iron can(c) wrapped with insulation around it when passingcurrent through it(d) placed inside an aluminium can (1998)5.7 Permanent Magnets and Electromagnets34. Electromagnets are made of soft iron because softiron has(a) low retentivity and high coercive force(b) high retentivity and high coercive force(c) low retentivity and low coercive force(d) high retentivity and low coercive force(2010)ANSWER KEY1. (d) 2. (b) 3. (c) 4. (d) 5. (a) 6. (b) 7. (b) 8. (d) 9. (a) 10. (c)11. (b) 12. (b) 13. (a) 14. (a,d) 15. (d) 16. (c) 17. (d) 18. (d) 19. (b) 20. (b)21. (a) 22. (a) 23. (c) 24. (a) 25. (d) 26. (d) 27. (c) 28. (d) 29. (a) 30. (a)31. (a) 32. (a) 33. (b) 34. (c)Hints & Explanations1. (d) : Work done in a coilW = mB (cosq 1 – cosq 2 )When it is rotated by angle 180° thenW = 2mB = 2 (NIA)BGiven: N = 250, I = 85 mA = 85 × 10 –6 AA = 1.25 × 2.1 × 10 –4 m 2 ≈ 2.6 × 10 –4 m 2...(i)B = 0.85 TPutting these values in eqn. (i), we getW = 2 × 250 × 85 × 10 –6 × 2.6 × 10 –4 × 0.85≈ 9.1 × 10 –6 J = 9.1 mJ2. (b) : At equilibrium, potential energy of dipoleU i = – MB H

Telegram @unacademyplusdiscounts54 NEET-AIPMT Chapterwise Topicwise Solutions PhysicsFinal potential energy of dipole,MBHUf=− MBHcos60°=−2MBHMBHW = Uf− Ui=− −− ( MBH) =...(i)2 2τ= MBH sin60 °= 2 3W × [Using eqn. (i)]2= 3W3. (c) : The direction of magnetic dipole moment is fromsouth to north pole of the magnet.In configuration (1),mnet = 2m + 2m + 2mmcos90°2 2= m + m = mIn configuration (2),2m net = m – m = 0In configuration (3),m net = 2m + 2m + 2mmcos30 °2 2 ⎛ ⎞= 2m + 2m ⎝⎜3⎠ ⎟ = m 2+32In configuration (4),mnet = 2m + 2m + 2mmcos60°2 2 ⎛= 2m + 2m 1⎝⎜ ⎞ ⎠ ⎟ = m 324. (d) : Let m be strength of each pole of bar magnet oflength l. ThenM = m × l...(i)When the bar magnet is bent in the form of an arc asshown in figure. Thenπ πrl= × r =3 3 or r l= 3 πNew magnetic dipole momentM′ = m × 2r sin30°= m × 2 × 3 l ml M× 1 3 32 = = (Using (i))π π π5. (a)6. (b) : Work done in changing the orientation of amagnetic needle of magnetic moment M in a magneticfield B from position q 1 to q 2 is given byW = MB(cosq 1 – cosq 2 )Here, q 1 = 0°, q 2 = 60°= MB ⎛ ⎞−⎝⎜⎠⎟ = MB1 1 ...(i)2 2The torque on the needle is τ= M × BIn magnitude,3τ= MBsinθ= MBsin60°=MB...(ii)2Dividing (ii) by (i), we getτ=W3 or τ= 3W = 3 × 3J = 7. (b) : Here, Magnetic moment, M = 0.4 J T –1Magnetic field, B = 0.16 TWhen a bar magnet of magnetic moment is placed in auniform magnetic field , its potential energy isU =−M⋅ B=−MBcosθFor stable equilibrium, q = 0°\ U = –MB = –(0.4 J T –1 )(0.16 T) = –0.064 J8. (d) : The time period T of oscillation of a magnet isgiven byT = 2πIMBwhere,I = Moment of inertia of the magnet about the axis ofrotationM = Magnetic moment of the magnetB = Uniform magnetic fieldAs I and M remain the same1 T2B1∴ T ∝ or =B T1B2According to given problem,B 1 = 24 mT, B 2 = 24 mT – 18 mT = 6 mT, T 1 = 2 s( 24 µ T)∴ T 2 = ( 2 s)= 4 s( 6 µ T)9. (a) : Magnetic field due to bar magnets exerts forceon moving charges only. Since the charge is at rest, noforce acts on it.10. (c) : Magnetic moment of the loopM = NIA = 2000 × 2 × 1.5 × 10 –4 = 0.6 J/TTorque t = MBsin30°= × × − 2 1 −206 . 5 10 × = 15 . × 10 Nm211. (b) : Here, M = 2 × 10 4 J T –1B = 6 × 10 –4 T, q 1 = 0°, q 2 = 60°W = MB(cosq 1 – cosq 2 ) = MB(1 – cos60°)4 −4⎛ ⎞W = 2× 10 × 6× 10 −⎝⎜1 1 ⎠⎟2= 6 J.12. (b) : Initial mass of the magnet (m 1 ) = m and finalmass of the magnet (m 2 ) = 4m.2I mkThe time period, T = 2π = 2π∝ mMB MBTherefore T 1 m1m 1= = =T2m2 4m2or T 2 = 2T 1 = 2T13. (a) :

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54 NEET-AIPMT Chapterwise Topicwise Solutions Physics

Final potential energy of dipole,

MBH

Uf

=− MBH

cos60°=−

2

MBH

MBH

W = Uf

− Ui

=− −− ( MBH) =

...(i)

2 2

τ= MBH sin60 °= 2 3

W × [Using eqn. (i)]

2

= 3W

3. (c) : The direction of magnetic dipole moment is from

south to north pole of the magnet.

In configuration (1),

mnet = 2

m + 2

m + 2mmcos90

°

2 2

= m + m = m

In configuration (2),

2

m net = m – m = 0

In configuration (3),

m net = 2

m + 2

m + 2mmcos

30 °

2 2 ⎛ ⎞

= 2m + 2m ⎝

3

⎠ ⎟ = m 2+

3

2

In configuration (4),

mnet = 2

m + 2

m + 2mmcos60

°

2 2 ⎛

= 2m + 2m 1

⎜ ⎞ ⎠ ⎟ = m 3

2

4. (d) : Let m be strength of each pole of bar magnet of

length l. Then

M = m × l

...(i)

When the bar magnet is bent in the form of an arc as

shown in figure. Then

π πr

l= × r =

3 3 or r l

= 3 π

New magnetic dipole moment

M′ = m × 2r sin30°

= m × 2 × 3 l ml M

× 1 3 3

2 = = (Using (i))

π π π

5. (a)

6. (b) : Work done in changing the orientation of a

magnetic needle of magnetic moment M in a magnetic

field B from position q 1 to q 2 is given by

W = MB(cosq 1 – cosq 2 )

Here, q 1 = 0°, q 2 = 60°

= MB ⎛ ⎞

⎟ = MB

1 1 ...(i)

2 2

The torque on the needle is

τ= M × B

In magnitude,

3

τ= MBsinθ= MBsin60°=

MB

...(ii)

2

Dividing (ii) by (i), we get

τ

=

W

3 or τ= 3W = 3 × 3J = 7. (b) : Here, Magnetic moment, M = 0.4 J T –1

Magnetic field, B = 0.16 T

When a bar magnet of magnetic moment is placed in a

uniform magnetic

field , its potential energy is

U =−M⋅ B=−MB

cosθ

For stable equilibrium, q = 0°

\ U = –MB = –(0.4 J T –1 )(0.16 T) = –0.064 J

8. (d) : The time period T of oscillation of a magnet is

given by

T = 2π

I

MB

where,

I = Moment of inertia of the magnet about the axis of

rotation

M = Magnetic moment of the magnet

B = Uniform magnetic field

As I and M remain the same

1 T2

B1

∴ T ∝ or =

B T1

B2

According to given problem,

B 1 = 24 mT, B 2 = 24 mT – 18 mT = 6 mT, T 1 = 2 s

( 24 µ T)

∴ T 2 = ( 2 s)

= 4 s

( 6 µ T)

9. (a) : Magnetic field due to bar magnets exerts force

on moving charges only. Since the charge is at rest, no

force acts on it.

10. (c) : Magnetic moment of the loop

M = NIA = 2000 × 2 × 1.5 × 10 –4 = 0.6 J/T

Torque t = MBsin30°

= × × − 2 1 −2

06 . 5 10 × = 15 . × 10 Nm

2

11. (b) : Here, M = 2 × 10 4 J T –1

B = 6 × 10 –4 T, q 1 = 0°, q 2 = 60°

W = MB(cosq 1 – cosq 2 ) = MB(1 – cos60°)

4 −4

⎛ ⎞

W = 2× 10 × 6× 10 −

⎜1 1 ⎠

2

= 6 J.

12. (b) : Initial mass of the magnet (m 1 ) = m and final

mass of the magnet (m 2 ) = 4m.

2

I mk

The time period, T = 2π = 2π

∝ m

MB MB

Therefore T 1 m1

m 1

= = =

T2

m2 4m

2

or T 2 = 2T 1 = 2T

13. (a) :

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