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:
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:
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
Here,
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
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:
The force balance equation:
Substituting the given values:
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:
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:
The magnetic energy as a function of time is:
μ = 1/2 L i02 (1 - e-Rt/L)2
Where:
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:
The centripetal force required for circular motion is:
F = m v2 / r
Where:
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 0.1Am2 from 0° to 90° in a field of 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:
For a circular loop, the area A can be calculated as:
A = π r2
Given:
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
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