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Numerical Problems: Moving Charges and Magnetism | Physics Class 12 - NEET PDF Download

Q1. A wire bent in the form of a sector of radius r subtending an angle θ° at the center carries a current i. The magnetic field at the center O is:

Sol: The magnetic field at the center of a complete circular loop carrying current i is given by:

Bfull = μ0i/2r

where:
μ0 = permeability of free space
i = current in the wire
r = radius of the loop

For a circular sector that subtends an angle θ° at the center:

  1. The sector represents a fraction θ/360 of the full circle
  2. The magnetic field is proportionally reduced by this fraction
Bsector = (θ/360) × Bfull = (θ/360) × (μ0i/2r)

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Q2. A conducting wire bent in the form of a parabola y2 = 2x carries a current i = 2A. This wire is placed in a uniform magnetic field B = -4k tesla. The magnetic force on the wire is

Sol: FAOB = FAB = i (1 × B)

Here,

AB = 2√(2 × 2) = 4m
FAB= 2[ (-4i) × (-4k) ] = 32i

Q3. A paramagnetic material of magnetic susceptibility 2 × 10-5 is placed in magnetic field 0.1 × 10-4 A/m-1. The intensity of magnetization of material in unit A/m-1 is

Sol: xav = I/H ⇒ I = xa × H
= 2 × 10-5 × 0.1 × 10-4
= 2 × 10-10

Q4. A charged particle is moving in a circular orbit of radius 6 cm with a uniform speed of 3 × 106 m/s under the action of uniform magnetic field 2 × 10-4 Wb/m2 at right angles to the plane of the orbit. The charge to mass ratio of the particle is:

Sol: Given values:

v = 3 × 106 m/s-1
B = 2 × 10-4 Wb/m-2 = 2 × 10-4 T
R = 6 cm = 6 × 10-2 m

The force balance equation:

Bqv = mv2/R ⇒ q/m = v/(BR)

Substituting the given values:

q/m = (3 × 106) / (2 × 10-4 × 6 × 10-2)
= 0.25 × 1012 C/kg
= 2.5 × 1011C/kg

Q5. A short bar magnet produces a magnetic induction of 4 × 10-5 T at an axial point 10 cm from its centre. Its dipole moment is (μ0 = 4π × 10-7 Wb/Am)

Sol: At an axial point:

B = (μ0/4π) × (2M/r3)
4 × 10-5 = (10-7 × 2M) / 0.001
M = (4 × 10-5 × 0.001) / (2 × 10-7)
= 0.2 Am2

Q6. A solenoid has an inductance of 10 henry and a resistance of 2Ω. It is connected to a 10V battery. The time taken by the magnetic energy to reach (1/4) of its maximum value is

Sol: The magnetic energy (μ) stored in the solenoid is given by the formula:

μ = 1/2 L i2

Where:

  • L is the inductance (10 henry)
  • i is the current

The magnetic energy as a function of time is:

μ = 1/2 L i02 (1 - e-Rt/L)2

Where:

  • i0 is the maximum current
  • R is the resistance (2Ω)
  • t is the time

We need to find the time when μ reaches (1/4) of its maximum value. The maximum value of μ is 1/2 L i02, so (1/4) of the maximum value is:

μ' = 1/4

Therefore:

1 - e-Rt/L = 1/2

e-Rt/L = 1/2

Taking the natural logarithm on both sides:

-Rt/L = log 2

Since log 2 = 0.7 (given):

t = (L/R) log 2

Substituting the values L = 10 and R = 2:

t = (10/2) × 0.7

t = 5 × 0.7

t = 3.5 s

Q7. An electron with kinetic energy 5 keV enters a magnetic field of 0.01 T perpendicular to it. Find the radius of its path.

Sol: To find the radius of the electron's path, we use the relationship between the magnetic force and the centripetal force acting on the electron. The magnetic force provides the necessary centripetal force for circular motion.

The magnetic force on a charged particle is given by:

F = q v B

Where:

  • q is the charge of the electron (1.6 × 10-19 C)
  • v is the velocity of the electron
  • B is the magnetic field strength (0.01 T)

The centripetal force required for circular motion is:

F = m v2 / r

Where:

  • m is the mass of the electron (9.11 × 10-31 kg)
  • r is the radius of the path

Equating the magnetic force to the centripetal force:

q v B = m v2 / r

Solving for the radius r:

r = m v / (q B)

First, we need to find the velocity v of the electron using its kinetic energy. The kinetic energy (KE) is given as 5 keV. Converting keV to joules:

1 keV = 1.6 × 10-16 J

KE = 5 × 1.6 × 10-16 = 8 × 10-16 J

The kinetic energy is also given by:

KE = 1/2 m v2

Solving for v2:

v2 = 2 KE / m

v2 = 2 × (8 × 10-16) / (9.11 × 10-31)

v2 ≈ 1.76 × 1015

v ≈ √(1.76 × 1015) ≈ 4.19 × 107 m/s

Now substitute the values into the radius formula:

r = (m v) / (q B)

r = (9.11 × 10-31 × 4.19 × 107) / (1.6 × 10-19 × 0.01)

r = (3.82 × 10-23) / (1.6 × 10-21)

r ≈ 2.39 × 10-2 m

r ≈ 0.0239 m or 2.39 cm

Q8. Find the work done in rotating a magnetic dipole of 0.1\, \text{Am}^20.1Am2 from 0° to 90° in a field of 0.5 T0.5\, \text{T}T. 

Sol: Work Done = W = mB( cos(θ₁) - cos(θ₂) )

Substituting the values:

W = 0.1 × 0.5 × (cos(0°) - cos(90°))
W = 0.1 × 0.5 × (1 - 0) = 0.05 J

Q9. A circular loop of radius 10 cm carries a current of 5 A. We need to calculate the magnetic dipole moment.

Sol: The magnetic dipole moment (m) of a current-carrying loop is given by the formula:

m = I A

Where:

  • I is the current flowing through the loop (in amperes)
  • A is the area of the loop (in square meters)

For a circular loop, the area A can be calculated as:

A = π r2

Given:

  • Current (I) = 5 A
  • Radius (r) = 10 cm = 0.1 m

A = π  (0.1)2 = π (0.01) = 0.0314 m2 (approximating π as 3.14)

Now, substitute the values into the magnetic dipole moment formula:

m = I A = 5 × 0.0314 = 0.157 Am2

However, using the exact value of π and the provided solution, we can simplify the calculation as follows:

m = I  A = 5 π (0.1)2 = 5 π (0.01) = 5π × 10-2 = 0.157 Am2

Thus, the magnetic dipole moment is:

m = 0.157 Am

Q10. Find the magnetic field at a point on the axis at 20 cm from the center of a loop of radius 5 cm carrying 10 A current.

Sol: The magnetic field (B) at a distance x from the center of a circular loop of radius R carrying current I is given by:

B = (μ0 I R2) / (2(R2 + x2)3/2)

Where:
μ0 = 4π × 10-7 Tm/A (permeability of free space)
I = 10 A (current)
R = 5 cm = 0.05 m (loop radius)
x = 20 cm = 0.2 m (distance from center)

Plugging in the values:

B = (4π × 10-7 × 10 × (0.05)2) / (2((0.05)2 + (0.2)2)3/2)

B ≈ 3.48 × 10-6 T

The document Numerical Problems: Moving Charges and Magnetism | Physics Class 12 - NEET is a part of the NEET Course Physics Class 12.
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FAQs on Numerical Problems: Moving Charges and Magnetism - Physics Class 12 - NEET

1. What is the principle of superposition in the context of magnetic fields?
Ans. The principle of superposition states that the resultant magnetic field at any point due to multiple magnetic sources is the vector sum of the individual magnetic fields produced by each source at that point. This means that if you have several charges or magnets, you can calculate the net magnetic field by adding the contributions from each source, taking into account their directions and magnitudes.
2. How does the direction of the magnetic field relate to the direction of the current in a wire?
Ans. The direction of the magnetic field around a straight current-carrying wire can be determined using the right-hand rule. If you point your thumb in the direction of the conventional current (from positive to negative), your fingers will curl in the direction of the magnetic field lines that encircle the wire. This relationship illustrates how electric currents produce magnetic fields.
3. What is the formula for calculating the magnetic force on a moving charge in a magnetic field?
Ans. The magnetic force \( F \) on a moving charge \( q \) can be calculated using the formula: \[ F = q(\mathbf{v} \times \mathbf{B}) \] where \( \mathbf{v} \) is the velocity of the charge and \( \mathbf{B} \) is the magnetic field. The force is a vector quantity, and the direction of the force can be determined using the right-hand rule for cross products.
4. What is the significance of the Lorentz force in the study of moving charges and magnetism?
Ans. The Lorentz force is the force experienced by a charged particle moving in an electromagnetic field. It is significant because it combines both electric and magnetic forces, and is given by the equation: \[ \mathbf{F} = q(\mathbf{E} + \mathbf{v} \times \mathbf{B}) \] This equation helps us understand how charges behave when they are subjected to electric fields and magnetic fields simultaneously, which is crucial in many applications, including electric motors and particle accelerators.
5. How do magnetic field lines behave around a magnet, and what do they represent?
Ans. Magnetic field lines are imaginary lines that represent the direction and strength of the magnetic field around a magnet. They emerge from the north pole and enter the south pole, showing that magnetic fields are directed from north to south outside the magnet. The density of these lines indicates the strength of the magnetic field; closer lines represent stronger fields, while farther lines indicate weaker fields.
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