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33 Years NEET-AIPMT Chapterwise Solutions - Physics 2020

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46 NEET-AIPMT Chapterwise Topicwise Solutions Physics

qvB

mv 2

m × 2π

= ⇒ qB = mω

=

R

T

2πm

∴ T = is independent of v and R.

qB

16. (a) : When a charged particle having K.E., T enters

in a field of magnetic induction, which is perpendicular

to its velocity, it takes a circular trajectory. It does not

increase in energy, therefore T is the K.E.

17. (a) : If a moving charged particle is subjected to a

perpendicular uniform magnetic field, then according to

F = qvB sinq, it will experience a maximum force which

will provide the centripetal force to particle and it will

describe a circular path with uniform speed.

18. (c) : The frequency of revolution of a charged

particle in a perpendicular magnetic field is

υ = 1 = 1

π = v

π = v

2 2 2π × eB

T r v r

= eB

/

mv 2πm

2

mv

19. (d) : qvB sinθ=

R

5

mv

R = qB

= 3×

10

= . =

sinθ

10 × 03 . ×

1 002m 2 cm

8

2

20. (b) : When a positively charged particle enters in a

region of uniform magnetic field, directed perpendicular

to the velocity it experiences a centripetal force which

will move it in circular path with a uniform speed.

⎛ 1 2 ⎞

21. (a) : Kinetic energy of electron ×

⎜ mv

2 ⎠

⎟ = 10 eV

and magnetic induction (B) = 10 –4 Wb/m 2

1 −31 2 −19

Therefore, ( 91 . × 10 ) v = 10 × ( 16 . × 10 )

2

(. )

or, v 2 19

2 10 1 6 10

12

= × × × −

= 352 . × 10

−31

91 . × 10

or, v = 1.876 × 10 6 m/s

Centripetal force, mv 2

= Bev

r

−31 6

mv ( 91 . × 10 ) × ( 1. 876 × 10 )

Therefore, r = =

Be −4 −19

10 × (. 16×

10 )

=11 × 10 –2 m = 11 cm

mv

22. (c) : r = or r ∝v

qB

As v is doubled, the radius also becomes doubled. Hence

new radius = 2 × 2 = 4 cm

23. (d) : For a charged particle orbiting in a circular

path in a magnetic field mv 2

Bqr

= Bvq ⇒ v=

r

m

E mv Bqvr Bq r Bqr 2 2 2

Bqr

K = 1 2

= 1

2 2 = 2 ⋅ m

= 2m

2 2 2

Bq × r

Fordeuteron, E1

=

2m

2 2 2

Bqr

For proton, E2

=

2m

E1

1 50 keV 1

= ⇒ = ⇒ E2

= 100 keV

E2 2 E2

2

24. (c) : Frequency, υ = eB m

or B = 2π υ

2πm

e

As mv 2

eBR

= evB or v = =2πυR

R

m

1 2 1

2

Kineticenergy, K = mv = m( 2πυ R)

= 2mp 2 u 2 R 2

2 2

25. (c)

26. (a) : Electron travelling in a magnetic field

perpendicular to its velocity follows a circular path.

27. (a) : In mass spectrometer when ions are accelerated

through potential V,

1 2

mv = qV

... (i)

2

where m is the mass of ion, q is the charge of the ion.

As the magnetic field curves the path of the ions in a

semicircular orbit

2

mv BqR

∴ Bqv = ⇒ v =

... (ii)

R

m

Substituting (ii) in (i), we get

2

1 ⎡

2

m BqR ⎤

q V

qV

2

m

⎣ ⎦

= or, m

= 2 2

BR

Since V, B are constants,

q

1 charge on the ion

or,

1

m 2 2

R mass of the ion

R

E

28. (a) : eE = evB ∴ v=

B

29. (d) : Electric field (E) = 20 V/m and magnetic field

(B) = 0.5 T.

The force on electron in a magnetic field = evB

Force on electron in an electric field = eE

Since the electron is moving with constant velocity,

therefore the resultant force on electron is zero.

i.e., eE = evB ⇒ v = E/B = 20/0.5 = 40 m s –1

30. (b) : According to Biot-Savart’s law,

⎛ dl r

× ⎞ µ 0 ⎛ dl × r ⎞

dB ∝ i ⎜ ⎟ or dB = i ⎜ ⎟.

⎝ 3

r ⎠ 4π

⎝ 3

r ⎠

31. (a) : Magnetic field due to i 1 = µ 01 i θ 1

2R 2π

(Into the plane)

Magnetic field due to

02 i 2

i2

= µ θ (Out of the plane)

2R

2π For parallel combination

Now, i 1 ρl2

A l2

= × =

i2

A ρl1

l1

1

i

R

⇒ 1 4 ( 2 π ) 1 i

= = ⇒

2

i1

= ⇒ i2 = 3i1

i 3

2 R

4 2 3 3

( π )

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