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JEE Main Physics: Moving Charges and Magnetism questions with solutions

194 questions with worked solutions.

Questions

Q1. A tightly wound solenoid has 2000 turns and a cross-sectional area of 1.5 × 10⁻⁴ m². It carries a current of 2.0 A and is hung at its center with its axis perpendicular to its length so that it can rotate in a horizontal plane. If it is placed in a uniform magnetic field of strength 5 × 10⁻² tesla, and the field makes an angle of 30° with the solenoid axis, what torque acts on the solenoid?

  1. 3 × 10⁻² N-m
  2. 3 × 10⁻³ N-m
  3. 1.5 × 10⁻³ N-m
  4. 1.5 × 10⁻² N-m

Answer: 1.5 × 10⁻² N-m

tau = N*I*A*B*sin(30) = 2000 * 2.0 * 1.5e-4 * 5e-2 * 0.5 = 1.5e-2 N-m.

Q2. A cyclotron with dee radius R is used to speed up protons of mass m. An alternating electric field of frequency ν is applied across the dees. For the cyclotron to operate, the magnetic field B and the kinetic energy K of the emerging proton beam are related by:

  1. B = mν / e and K = 2mπ²ν²R²
  2. B = 2πmν / e and K = m²πνR²
  3. B = 2πmν / e and K = 2mπ²ν²R²
  4. B = mν / e and K = m²πνR²

Answer: B = 2πmν / e and K = 2mπ²ν²R²

Cyclotron resonance: nu = eB/(2 pi m) so B = 2 pi m nu/e. v_max = 2 pi nu R, so K = (1/2)m(2 pi nu R)^2 = 2 m pi^2 nu^2 R^2.

Q3. A long, straight conductor of radius a carries a constant current I that is spread uniformly over its cross-sectional area. What is the ratio of the magnetic field at a distance a/2 from the axis to the magnetic field at a distance 2a from the axis?

  1. 1/2
  2. 1/4
  3. 4
  4. 1

Answer: 1

The magnetic field inside a long, straight conductor increases linearly with distance from the center, while outside the conductor, it decreases with the distance from the axis. At a distance a/2, the magnetic field is proportional to the distance from the center, while at 2a, it behaves inversely with distance, leading to a ratio of 1.

Q4. A charge of 2 μC revolves with a frequency of 6.25 × 10¹² Hz and creates a magnetic field of 6.28 T at a point on the circle. What is the radius of the circular path?

  1. 2.25 m
  2. 0.25 m
  3. 13.0 cm
  4. 1.25 m

Answer: 1.25 m

I = q*f = 2e-6 * 6.25e12 = 1.25e7 A. From B = mu0*I/(2r), r = mu0*I/(2B) = (4*pi*1e-7 * 1.25e7)/(2*6.28) = 1.25 m.

Q5. An electron beam travels through a region where uniform electric and magnetic fields act mutually perpendicular to each other, and both are also perpendicular to the direction of motion of the electrons. If the electric field strength is 20 V m−1 and the magnetic field strength is 0.5 T, the speed of the electrons must be

  1. 8 m/s
  2. 20 m/s
  3. 40 m/s
  4. 1/40 m/s

Answer: 40 m/s

For undeflected motion the electric and magnetic forces balance: qE = qvB, so v = E/B = 20/0.5 = 40 m/s.

Q6. A particle having mass m and charge q is first accelerated through a potential difference V and then enters a zone of uniform magnetic field B acting perpendicular to its velocity. If the magnetic field extends over a width d, what is the angle through which the particle’s direction changes on emerging from the field?

  1. sin−1[ Bd (q/2mV)1/2 ]
  2. cos−1[ Bd (q/2mV)1/2 ]
  3. tan−1[ Bd (q/2mV)1/2 ]
  4. zero

Answer: sin−1[ Bd (q/2mV)1/2 ]

From qV=(1/2)mv^2, v=sqrt(2qV/m); radius r=mv/(qB). Deflection angle theta has sin(theta)=d/r = Bd*(q/(2mV))^(1/2), so theta = sin^-1[Bd(q/2mV)^(1/2)].

Q7. A charged particle of charge q and mass m is moving in a circular path of radius r with angular velocity ω. The ratio of the magnitude of its magnetic moment to the magnitude of its angular momentum depends on

  1. ω and q
  2. ω, q and m
  3. q and m
  4. ω and m

Answer: q and m

Magnetic moment = (1/2)*q*omega*r^2 and angular momentum = m*omega*r^2, so their ratio = q/(2m), which depends only on q and m.

Q8. In a mass spectrometer, ions are first accelerated through a potential difference V and then forced by a magnetic field B to move along a semicircular path of radius R. If V and B remain unchanged, how does the charge-to-mass ratio of the ion vary with R?

  1. It is proportional to 1/R²
  2. It is proportional to R²
  3. It is proportional to R
  4. It is proportional to 1/R

Answer: It is proportional to 1/R²

From qV = (1/2)mv^2 and R = mv/(qB): q/m = 2V/(R^2 B^2), so q/m is proportional to 1/R^2.

Q9. A long straight wire carrying a constant current is shaped first into a single-turn circular loop, producing a magnetic field of magnitude B at its centre. If the same wire, with the same current, is instead wound into a circular coil of n turns having a smaller radius, what will be the magnetic field at the centre?

  1. B/n
  2. nB
  3. B/n²
  4. n²B

Answer: n²B

When the wire is wound into a coil with n turns, the magnetic field at the center increases because each turn contributes to the total magnetic field. The magnetic field strength is proportional to the number of turns squared, resulting in a field strength of n²B at the center.

Q10. A charged particle enters a magnetic field with its velocity at right angles to the field. Its motion will be such that

  1. its kinetic energy varies, while its momentum remains unchanged
  2. its momentum varies, while its kinetic energy remains unchanged
  3. neither its momentum nor its kinetic energy stays constant
  4. both its momentum and its kinetic energy stay constant

Answer: its momentum varies, while its kinetic energy remains unchanged

The magnetic force is perpendicular to velocity, so it does no work: kinetic energy (and speed) stay constant. Momentum is a vector whose direction continuously changes, so momentum varies.

Q11. A charged particle starts from rest in a region where uniform, time-independent electric and magnetic fields are present and both fields point in the same direction. The particle’s path will be

  1. a straight path
  2. a circular path
  3. a helical path
  4. a cycloidal path

Answer: a straight path

From rest, only E acts initially, accelerating the particle along B. Since the velocity stays parallel to B, the magnetic force qv x B is always zero, so the path is a straight line along the field.

Q12. An equilateral triangular coil of side l is placed between the pole pieces of a permanent magnet so that the magnetic field B lies in the plane of the coil. If a current i flowing through the triangle produces a torque τ on it, then the side length l of the triangle is

  1. (2/√3)(τ/Bl)
  2. 2(τ/√3Bl)^(1/2)
  3. (2/√3)(τ/Bl)^(1/2)
  4. (1/√3)(τ/Bl)

Answer: 2(τ/√3Bl)^(1/2)

With B in the coil's plane, torque tau = i*A*B = i*(sqrt3/4)*l^2*B. Solving, l = 2*sqrt(tau/(sqrt3 * B * i)), which is index 1.

Q13. A magnetic needle is placed in a magnetic field that is not uniform. What will it experience?

  1. No force and no torque
  2. Torque only, not force
  3. Force only, not torque
  4. Both force and torque

Answer: Both force and torque

In a non-uniform magnetic field, the magnetic needle experiences a gradient in the magnetic field strength, which results in both a force acting on it and a torque that tends to align it with the field. The force arises from the variation in magnetic field strength across the needle, while the torque is due to the interaction of the needle's magnetic moment with the field.

Q14. A dead-beat galvanometer shows a pointer that quickly comes to rest at a fixed reading because

  1. eddy currents are set up in the metallic frame supporting the coil.
  2. the magnet used in it has a very high strength.
  3. the pointer attached to it has negligible mass.
  4. the supporting frame is made of ebonite.

Answer: eddy currents are set up in the metallic frame supporting the coil.

A dead-beat galvanometer has its coil wound on a metallic (conducting) frame; the induced eddy currents oppose the motion, quickly damping oscillations so the pointer settles fast.

Q15. When an electric current flows through a spring, what happens to it?

  1. It expands
  2. It contracts
  3. It stays unchanged
  4. None of the above

Answer: It contracts

When an electric current flows through a spring, it generates heat due to resistance, causing the material to expand initially but then contract as it cools down, resulting in an overall contraction.

Q16. A circular loop A has radius R and carries a current I. Another circular loop B has radius 2R and carries a current 2I. What is the ratio of the magnetic field strengths produced at their centers, B_A: B_B?

  1. 1
  2. 2
  3. 1/2
  4. 4

Answer: 1

The magnetic field at the center of a circular loop is directly proportional to the current and inversely proportional to the radius. For loop A, the field is proportional to I/R, and for loop B, it is proportional to (2I)/(2R). Simplifying both expressions shows that they are equal, resulting in a ratio of 1.

Q17. An electron and a proton, each with the same momentum, enter a uniform magnetic field at right angles to the field. What will be the nature of their paths?

  1. Their trajectories will have the same curvature, apart from the direction of rotation.
  2. Neither particle will be deflected.
  3. The electron’s trajectory will be more sharply curved than the proton’s.
  4. The proton’s trajectory will be more sharply curved than the electron’s.

Answer: Their trajectories will have the same curvature, apart from the direction of rotation.

Both the electron and the proton experience the same magnetic force due to their equal momentum and perpendicular entry into the magnetic field, resulting in circular paths. However, the electron, being lighter, will have a faster angular velocity, leading to the same curvature but opposite rotation direction.

Q18. For a charged particle moving in a circle inside a uniform magnetic field, the time period does not depend on its

  1. speed
  2. mass
  3. charge
  4. magnetic field strength

Answer: speed

The time period of a charged particle moving in a magnetic field is determined by the radius of the circular path and the magnetic field strength, and it remains constant regardless of the particle's speed. This is because the magnetic force provides the necessary centripetal force, leading to a fixed frequency of rotation.

Q19. A particle having mass M and charge Q moves with speed v in a uniform magnetic field B applied perpendicular to its velocity, so that it traces a circle of radius R. The total work done by the magnetic field during one complete revolution is

  1. (Mv²/R) 2πR
  2. zero
  3. BQ2πR
  4. BQv2πR

Answer: zero

The work done by a magnetic field on a charged particle is always zero because the magnetic force acts perpendicular to the velocity of the particle, resulting in no displacement in the direction of the force.

Q20. A long conductor carries a constant current. When it is shaped into a single-turn circular loop, the magnetic field at the centre is B. If the same wire is then formed into a circular coil having n turns, the magnetic field at the centre becomes

  1. 2nB
  2. n²B
  3. nB
  4. 2n²B

Answer: n²B

Fixed wire length L = 2*pi*R. With n turns each radius r = R/n. B' = n*mu0*I/(2r) = n*mu0*I/(2R/n) = n^2 * mu0*I/(2R) = n^2 B.

Q21. A circular wire loop of radius 3 cm carries a current. The magnetic field produced by it at a point on its axis 4 cm from the centre is 54 μT. What is the magnetic field at the centre of the loop?

  1. 125 μT
  2. 150 μT
  3. 250 μT
  4. 75 μT

Answer: 250 μT

B_centre = B_axis*(R^2+x^2)^(3/2)/R^3 = 54*(3^2+4^2)^(3/2)/3^3 = 54*125/27 = 250 microT.

Q22. Two very long parallel wires are a distance d apart and carry currents I1 and I2 in the same direction, producing a mutual force of magnitude F. If the current in one wire is changed to twice its original value and its direction is reversed, while the separation is increased to 3d, what is the new force between the wires?

  1. -2F/3
  2. F/3
  3. -2F
  4. -F/3

Answer: -2F/3

F = mu0*I1*I2/(2*pi*d). Doubling one current and tripling the separation scales the magnitude by 2/3, and reversing that current flips attraction to repulsion (sign change). New force = -2F/3.

Q23. Two circular coils are concentric, each having a radius of 2π cm, and the planes of the coils are mutually perpendicular. If currents of 3 A and 4 A flow through the two coils, respectively, what is the magnitude of the magnetic induction at the common centre? Take μ0 = 4π × 10⁻⁷ Wb/A·m.

  1. 10⁻⁵
  2. 12 × 10⁻⁵
  3. 7 × 10⁻⁵
  4. 5 × 10⁻⁵

Answer: 5 × 10⁻⁵

The magnetic induction at the center of two perpendicular coils can be calculated using the formula for the magnetic field due to a circular coil, which is proportional to the current and inversely proportional to the radius. By applying the formula for both coils and considering their perpendicular arrangement, the resultant magnetic induction is found to be 5 × 10⁻⁵ Wb/m².

Q24. A particle with mass m and charge q moves in a circle of radius r in a plane perpendicular to a magnetic field of magnitude B. The period of one complete revolution is

  1. 2πq²B/m
  2. 2πmq/B
  3. 2πm/qB
  4. 2πqB/m

Answer: 2πm/qB

The period of revolution for a charged particle in a magnetic field is derived from the balance of the magnetic force and the centripetal force, leading to the formula T = 2πm/(qB), where T is the period, m is the mass, q is the charge, and B is the magnetic field strength.

Q25. Two very long, thin, parallel conductors are placed a distance d apart. If each carries the same current i in the same direction, then they will

  1. repel one another with a force of μ0i²/(2πd)
  2. attract one another with a force of μ0i²/(2πd)
  3. repel one another with a force of μ0i²/(2πd²)
  4. attract one another with a force of μ0i²/(2πd²)

Answer: attract one another with a force of μ0i²/(2πd)

Two long parallel wires carrying current in the same direction attract each other, with force per unit length F/L = mu0*i^2/(2*pi*d).

Q26. A charged particle is set free from rest in a region where constant, uniform electric and magnetic fields exist and both fields point in the same direction. The particle will move along a

  1. helical path
  2. straight path
  3. elliptical path
  4. circular path

Answer: straight path

The charge starts at rest, so qE accelerates it along E, which is parallel to B. Its velocity stays parallel to B, making qv x B = 0 at all times. It therefore moves in a straight line.

Q27. A long solenoid has a winding density of 200 turns per cm and carries a current i. The magnetic field at its centre is 6.28 × 10⁻² Weber/m². A second long solenoid has 100 turns per cm and carries a current i/3. What magnetic field is produced at its centre?

  1. 1.05 × 10⁻² Weber/m²
  2. 1.05 × 10⁻⁵ Weber/m²
  3. 1.05 × 10⁻³ Weber/m²
  4. 1.05 × 10⁻⁴ Weber/m²

Answer: 1.05 × 10⁻² Weber/m²

B = mu0*n*i, so B2 = B1*(n2/n1)*(i2/i1) = 6.28e-2*(100/200)*(1/3) = 1.05e-2 Wb/m^2.

Q28. A long, straight conductor of radius a carries a constant current i that is spread uniformly over its cross-sectional area. What is the ratio of the magnetic field magnitude at a distance a/2 from the axis to that at a distance 2a from the axis?

  1. 1/2
  2. 1/4
  3. 4
  4. 1

Answer: 1

At a/2 (inside): B = mu0*i*(a/2)/(2*pi*a^2) = mu0*i/(4*pi*a). At 2a (outside): B = mu0*i/(2*pi*2a) = mu0*i/(4*pi*a). The two are equal, so the ratio is 1.

Q29. A current I flows along the length of an infinitely long, straight, thin walled pipe. Then

  1. the magnetic field at all points inside the pipe is the same, but not zero
  2. the magnetic field is zero only on the axis of the pipe
  3. the magnetic field is different at different points inside the pipe
  4. the magnetic field at any point inside the pipe is zero

Answer: the magnetic field at any point inside the pipe is zero

According to Ampère's law and the properties of magnetic fields generated by current-carrying conductors, the magnetic field inside a hollow conductor is zero due to the symmetry of the current distribution, which results in the cancellation of the magnetic field lines.

Q30. A charged particle with charge q enters a region of constant, uniform, and mutually orthogonal fields E and B with a velocity v perpendicular to both E and B and comes out without any change in magnitude or direction of v. Then

  1. v = B × E / E²
  2. v = E × B / B²
  3. v = B × E / B²
  4. v = E × B / E²

Answer: v = E × B / B²

The correct option is derived from the condition that the net force acting on the charged particle must be zero for it to maintain its velocity. In a uniform electric field E and magnetic field B, the electric force qE and the magnetic force q(v × B) must balance each other, leading to the relationship v = E × B / B².

Q31. A charged particle moves through a magnetic field perpendicular to its direction. Then

  1. kinetic energy changes but the momentum is constant
  2. the momentum changes but the kinetic energy is constant
  3. both momentum and kinetic energy of the particle are not constant
  4. both momentum and kinetic energy of the particle are constant

Answer: the momentum changes but the kinetic energy is constant

When a charged particle moves through a magnetic field perpendicular to its velocity, the magnetic force acts as a centripetal force, changing the direction of the particle's momentum without altering its speed. Since the speed remains constant, the kinetic energy, which depends on speed, also remains constant.

Q32. A current I flows in an infinitely long wire with cross section in the form of a semi-circular ring of radius R. The magnitude of the magnetic induction along its axis is:

  1. (a) μ0I / 2π2R
  2. (b) μ0I / 2πR
  3. (c) μ0I / 4πR
  4. (d) μ0I / π2R

Answer: (d) μ0I / π2R

The magnetic induction along the axis of a semi-circular wire can be derived using the Biot-Savart law, which shows that the contribution to the magnetic field from each segment of the wire adds up to yield the result of μ0I / π2R. This reflects the unique geometry of the semi-circular shape, which influences the field strength along the axis.

Q33. A positive charge +q travels with velocity v = 3î + 4ĵ + k̂ in a region where the electric field is E = 3î + ĵ + 2k̂ and the magnetic field is B = î + ĵ − 3k̂. What is the y-component of the force acting on the charge?

  1. 11 q
  2. 5 q
  3. 3 q
  4. 2 q

Answer: 11 q

v x B = (3,4,1) x (1,1,-3) = (-13,10,-1). E + v x B = (-10,11,1). The force is q times this, so the y-component is 11q.

Q34. Proton, deuteron and alpha particle of same kinetic energy are moving in circular trajectories in a constant magnetic field. The radii of proton, deuteron and alpha particle are respectively rₚ, r_d and r_α. Which one of the following relation is correct?

  1. (a) r_α = rₚ = r_d
  2. (b) r_α = rₚ < r_d
  3. (c) r_α < r_d > rₚ
  4. (d) r_α > r_d > rₚ

Answer: (b) r_α = rₚ < r_d

For equal KE, r = sqrt(2mE)/(qB) ~ sqrt(m)/q. Proton: sqrt(1)/1=1; deuteron: sqrt(2)/1=1.41; alpha: sqrt(4)/2=1. Hence r_alpha = r_p < r_d (option b).

Q35. Two long coaxial solenoids of unequal radii carry the same current I in the same sense. Let F₁ denote the magnetic force on the inner solenoid due to the outer solenoid, and F₂ denote the magnetic force on the outer solenoid due to the inner solenoid. Which statement is correct?

  1. F₁ is directed radially inward and F₂ = 0
  2. F₁ is directed radially outward and F₂ = 0
  3. F₁ = F₂ = 0
  4. F₁ is directed radially inward and F₂ is directed radially outward

Answer: F₁ = F₂ = 0

The magnetic fields inside coaxial solenoids do not exert forces on each other when they carry the same current in the same direction, resulting in zero net force on both solenoids.

Q36. Two wires A and B are identical, each having length l and carrying the same current I. Wire A is shaped into a circular loop of radius R, while wire B is bent into a square of side a. If the magnetic fields at the centers of the circle and the square are BA and BB respectively, what is the value of BA/BB?

  1. π²/16
  2. π²/(8√2)
  3. π²/8
  4. π²/(16√2)

Answer: π²/(8√2)

The magnetic field at the center of a circular loop is given by the formula B = (μ₀I)/(2R), while for a square loop, it can be derived to be B = (μ₀I)/(4a) multiplied by a correction factor due to the geometry. Given that the side length a of the square is related to the radius R of the circle, the ratio BA/BB simplifies to π²/(8√2), making option B the correct answer.

Q37. An electron, a proton and an alpha particle having the same kinetic energy are moving in circular orbits of radii rₑ, rₚ and r_α respectively in a uniform magnetic field B. The relation between rₑ, rₚ, r_α is

  1. rₑ < rₚ = r_α
  2. rₑ < rₚ < r_α
  3. rₑ < r_α < rₚ
  4. rₑ = r_α < rₚ

Answer: rₑ < rₚ = r_α

The radius of the circular orbit in a magnetic field is directly proportional to the momentum of the particle and inversely proportional to its charge. Since the electron has a much smaller mass and charge compared to the proton and alpha particle, it will have a smaller radius for the same kinetic energy, leading to the relation rₑ < rₚ = r_α, as both the proton and alpha particle have the same charge-to-mass ratio.

Q38. The dipole moment of a circular loop carrying current I, is m and the magnetic field at the centre of the loop is B1. When the dipole moment is doubled by keeping the current constant, the magnetic field at the centre of the loop is B2. The ratio B1/B2 is

  1. 2
  2. √3
  3. √2
  4. 1/√2

Answer: √2

The magnetic dipole moment of a circular loop is directly proportional to the current and the area of the loop. When the dipole moment is doubled while keeping the current constant, the area must also double, leading to an increase in the magnetic field strength at the center of the loop by a factor of √2, resulting in the ratio B1/B2 being √2.

Q39. A rectangular coil (Dimension 5 cm × 2.5 cm) with 100 turns, carrying a current of 3 A in the clockwise direction, is kept centered at the origin and in the X-Z plane. A magnetic field of 1 T is applied along X-axis. If the coil is tilted through 45° about Z-axis, the torque on the coil is:

  1. 0.38 Nm
  2. 0.55 Nm
  3. 0.42 Nm
  4. 0.27 Nm

Answer: 0.27 Nm

m = N*i*A = 100*3*(0.05*0.025) = 0.375 A m^2. With coil in X-Z plane its normal is along Y (perpendicular to B along X). Tilting 45 deg about Z makes the angle between m and B equal 45 deg, so tau = m*B*sin45 = 0.375*1*0.707 = 0.27 Nm.

Q40. A current of 1A is flowing on the sides of an equilateral triangle of side 4.5 × 10⁻² m. The magnetic field at the center of the triangle will be -

  1. 4 × 10⁻⁵ Wb/m²
  2. Zero
  3. 2 × 10⁻⁵ Wb/m²
  4. 8 × 10⁻⁵ Wb/m²

Answer: 4 × 10⁻⁵ Wb/m²

For an equilateral triangle, perpendicular distance from centre to a side d = a/(2*sqrt(3)). Field from one side = (mu0*I/4pi/d)*2*sin60. With a=4.5e-2 m, I=1 A, each side gives ~1.33e-5 T; three sides total ~4e-5 Wb/m^2.

Q41. A particle having the same charge as of electron moves in a circular path of radius 0.5 cm under the influence of a magnetic field of 0.5 T. If an electric field of 100 V/m makes it to move in a straight path, then the mass of the particle is (Given charge of electron = -1.6 × 10⁻¹⁹ C)

  1. 1.6 × 10⁻¹⁹ kg
  2. 1.6 × 10⁻²⁷ kg
  3. 9.1 × 10⁻³¹ kg
  4. 2.0 × 10⁻²⁴ kg

Answer: 2.0 × 10⁻²⁴ kg

Straight-line motion needs qE=qvB so v=E/B=100/0.5=200 m/s. From r=mv/(qB), m=qBr/v=(1.6e-19*0.5*0.005)/200 = 2.0e-24 kg.

Q42. A proton, an electron, and a helium nucleus have the same energy. They are in circular orbits in a plane due to a magnetic field perpendicular to the plane. Let rₚ, rₑ and r_he be their respective radii. Then:

  1. rₑ < rₚ < r_he
  2. rₑ > rₚ = r_he
  3. rₑ < rₚ = r_he
  4. rₑ > rₚ > r_he

Answer: rₑ < rₚ = r_he

For equal energy, r = sqrt(2mE)/(qB) so r is proportional to sqrt(m)/q. For He: sqrt(4m_p)/2 = sqrt(m_p)/1 = same as proton, so r_p = r_he. The electron's tiny mass makes r_e the smallest, giving r_e < r_p = r_he.

Q43. A square loop is carrying a steady current I and the magnitude of its magnetic dipole moment is m. If this square loop is changed to a circular loop and it carries the same current, the magnitude of the magnetic dipole moment of circular loop will be:

  1. 4m/π
  2. 3m/π
  3. 2m/π
  4. m/π

Answer: 4m/π

Square side a gives m = I a^2 with perimeter 4a. Same wire forms a circle: 2*pi*r = 4a => r = 2a/pi, area = pi r^2 = 4a^2/pi. So m_circle = I*(4a^2/pi) = 4m/pi.

Q44. A rectangular coil (dimension 5 cm × 2.5 cm) with 100 turns, carrying a current of 3 A in the clock-wise direction, is kept centered at the origin and in the X-Z plane. A magnetic field of 1 T is applied along X-axis. If the coil is tilted through 45° about Z-axis, then the torque on the coil is -

  1. 0.55 N m
  2. 0.38 N m
  3. 0.42 N m
  4. 0.27 N m

Answer: 0.27 N m

The torque on a coil in a magnetic field is calculated using the formula τ = n * I * A * B * sin(θ), where n is the number of turns, I is the current, A is the area of the coil, B is the magnetic field strength, and θ is the angle between the magnetic field and the normal to the coil's plane. In this case, the area of the coil is 0.0125 m², the angle after tilting is 45°, and substituting these values gives the correct torque of 0.27 N m.

Q45. A moving coil galvanometer has a coil with 175 turns and area 1 cm². It uses a torsion band of torsion constant 10⁻⁶ N-m/rad. The coil is placed in a magnetic field B parallel to its plane. The coil deflects by 10° for a current of 1 mA. The value of B (in Tesla) is approximately:

  1. 10⁻³
  2. 10⁻¹
  3. 10⁻⁴
  4. 10⁻²

Answer: 10⁻²

The correct option is 10⁻² because the deflection angle of the coil is directly related to the magnetic field strength, the current, and the physical properties of the coil. Using the formula for torque in a galvanometer, we can derive that the magnetic field strength must be approximately 0.01 T to produce a 10° deflection at 1 mA.

Q46. In an experiment, electrons are accelerated, from rest, by applying a voltage of 500 V. Calculate the radius of the path if a magnetic field 100 mT is then applied. [Charge of the electron = 1.6 × 10⁻¹⁹ C, mass of the electron = 9.1 × 10⁻³¹ kg]

  1. 7.5 × 10⁻⁴ m
  2. 7.5 × 10⁻³ m
  3. 7.5 m
  4. 7.5 × 10⁻² m

Answer: 7.5 × 10⁻⁴ m

The correct option is right because the radius of the path of an electron in a magnetic field is determined by the balance between the centripetal force and the magnetic force acting on the electron. By calculating the velocity gained from the applied voltage and using the formula for the radius of circular motion in a magnetic field, the result yields a radius of 7.5 × 10⁻⁴ m.

Q47. A beam of protons with speed 4 × 10⁵ ms⁻¹ enters a uniform magnetic field of 0.3 T at an angle of 60° to the magnetic field. The pitch of the resulting helical path of protons is close to: (Mass of the proton = 1.67 × 10⁻²⁷ kg, charge of the proton = 1.69 × 10⁻¹⁹ C)

  1. 12 cm
  2. 4 cm
  3. 5 cm
  4. 2 cm

Answer: 4 cm

T = 2*pi*(1.67e-27)/(1.69e-19*0.3) = 2.07e-7 s. Pitch = v*cos60*T = 4e5*0.5*2.07e-7 = 0.041 m ~ 4 cm.

Q48. A charged particle carrying charge 1 μC is moving with velocity (2i + 3j + 4k) m/s. If an external magnetic field of (5i + 3j − 6k) × 10⁻³ T exists in the region where the particle is moving then the force on the particle is F × 10⁻⁹ N. The vector F is-

  1. (1) −3.0i + 3.2j − 0.9k
  2. (2) −300i + 320j − 90k
  3. (3) −30i + 32j − 9k
  4. (4) −0.30i + 0.32j − 0.09k

Answer: (3) −30i + 32j − 9k

v x B = (-30, 32, -9)*10^-3. F = q(v x B) = 10^-6 * (-30,32,-9)*10^-3 = (-30,32,-9)*10^-9 N, so F = -30i + 32j - 9k.

Q49. An electron is constrained to move along the y-axis with a speed of 0.1 c (c is the speed of light) in the presence of electromagnetic wave, whose electric field is E = 30 ĵ sin(1.5 × 10⁷ t − 5 × 10⁻² x) V/m. The maximum magnetic force experienced by the electron will be: (given c = 3 × 10⁸ m s⁻¹ and electron charge = 1.6 × 10⁻¹⁹ C)

  1. 1.6 × 10⁻¹⁹ N
  2. 4.8 × 10⁻¹⁹ N
  3. 3.2 × 10⁻¹⁸ N
  4. 2.4 × 10⁻¹⁸ N

Answer: 4.8 × 10⁻¹⁹ N

B_max = E_max/c = 30/(3e8) = 1e-7 T. v = 0.1c = 3e7 m/s. F = qvB = 1.6e-19 * 3e7 * 1e-7 = 4.8e-19 N.

Q50. A particle of charge q and mass m is moving with a velocity -v î (v ≠ 0) towards a large screen placed in the Y-Z plane at a distance d. If there is a magnetic field B = B0 k̂, the minimum value of v for which the particle will not hit the screen is:

  1. (1) qdB0/2m
  2. (2) 2qdB0/m
  3. (3) qdB0/3m
  4. (4) qdB0/m

Answer: (4) qdB0/m

The particle follows a circular arc whose maximum penetration toward the screen equals its radius r = mv/(qB0). It just fails to reach a screen at distance d when r = d, giving the critical speed v = qdB0/m.

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