Numerical Problems Based on Current Carrying Circular Loops for Class 12 Physics

  • Last modified on:2 months ago
  • Reading Time:11Minutes
Home CBSE Class 12 Physics Numerical Problems Current Carrying Circular Loops

Numerical Problems on Current Carrying Circular Loops

Class 12 Physics · Moving Charges and Magnetism
SQ

Magnetic Field of Circular Loops Practice Set

Apply $B = \frac{\mu_0 N I}{2R}$ and superposition principle
Ch 4 · Moving Charges and Magnetism
1
Consider a tightly wound 100 turn coil of radius 10 cm, carrying a current of 1 A. What is the magnitude of the magnetic field at the centre of the coil?
Answer $6.28 \times 10^{-4}\text{ T}$ 📝
Detailed Solution

Given parameters: Number of turns $N = 100$, Radius $R = 10\text{ cm} = 0.1\text{ m}$, Current $I = 1\text{ A}$.

The magnetic field at the centre of a circular coil is given by:

$$B = \frac{\mu_0 N I}{2R}$$

Substitute the values ($\mu_0 = 4\pi \times 10^{-7}\text{ T m/A}$):

$$B = \frac{4\pi \times 10^{-7} \times 100 \times 1}{2 \times 0.1} = \frac{4\pi \times 10^{-5}}{0.2}$$
$$B = 20\pi \times 10^{-5} = 2\pi \times 10^{-4}\text{ T}$$

Using $\pi \approx 3.14$:

$$B = 2 \times 3.14 \times 10^{-4} = 6.28 \times 10^{-4}\text{ T}$$
2
A circular loop of one turn carries a current of 5.0 A. If the magnetic field at the centre is 0.20 mT, find the radius of the loop.
Answer 1.57 cm 📝
Detailed Solution

Given: $N = 1$, Current $I = 5.0\text{ A}$, Magnetic field $B = 0.20\text{ mT} = 0.20 \times 10^{-3}\text{ T}$.

Using the formula $B = \frac{\mu_0 I}{2R}$, rearrange to solve for the radius $R$:

$$R = \frac{\mu_0 I}{2B}$$
$$R = \frac{4\pi \times 10^{-7} \times 5.0}{2 \times 0.20 \times 10^{-3}} = \frac{20\pi \times 10^{-7}}{0.40 \times 10^{-3}}$$
$$R = 50\pi \times 10^{-4}\text{ m} = 157.08 \times 10^{-4}\text{ m}$$

Convert meters to centimeters:

$$R = 1.5708 \times 10^{-2}\text{ m} \approx 1.57\text{ cm}$$
3
What current has to be maintained in a circular coil of wire of 50 turns and 2.54 cm in radius in order to just cancel the effect of earth’s magnetic field at a place where the horizontal component of earth’s field is $1.86 \times 10^{-5}\text{ T}$?
Answer 0.015 A 📝
Detailed Solution

To cancel the Earth’s magnetic field, the field produced by the coil at its centre must be equal and opposite to the horizontal component of the Earth’s field ($B_H$).

Given: $B = B_H = 1.86 \times 10^{-5}\text{ T}$, $N = 50$, $R = 2.54\text{ cm} = 2.54 \times 10^{-2}\text{ m}$.

$$B = \frac{\mu_0 N I}{2R} \implies I = \frac{2RB}{\mu_0 N}$$
$$I = \frac{2 \times (2.54 \times 10^{-2}) \times (1.86 \times 10^{-5})}{(4\pi \times 10^{-7}) \times 50}$$
$$I = \frac{9.4488 \times 10^{-7}}{200\pi \times 10^{-7}} = \frac{9.4488}{628.32}$$
$$I \approx 0.015\text{ A}$$
4
A semicircular arc of radius 20 cm carries a current of 10 A. Calculate the magnitude of the magnetic field at the centre of the arc.
Answer $1.57 \times 10^{-5}\text{ T}$ 📝
Detailed Solution

Radius $R = 20\text{ cm} = 0.2\text{ m}$, Current $I = 10\text{ A}$.

The magnetic field at the centre of a full circular loop is $\frac{\mu_0 I}{2R}$. For a semicircular arc, the magnetic field is exactly half of that of a full loop:

$$B = \frac{1}{2} \left( \frac{\mu_0 I}{2R} \right) = \frac{\mu_0 I}{4R}$$

Substitute the values:

$$B = \frac{4\pi \times 10^{-7} \times 10}{4 \times 0.2} = \frac{\pi \times 10^{-6}}{0.2}$$
$$B = 5\pi \times 10^{-6} \approx 5 \times 3.14 \times 10^{-6}$$
$$B \approx 15.7 \times 10^{-6}\text{ T} = 1.57 \times 10^{-5}\text{ T}$$
5

Two identical circular wires P and Q each of radius $R$ and carrying current $I$ are kept in perpendicular planes such that they have a common centre as shown in figure. Find the magnitude and direction of the net magnetic field at the common centre of the two coils.

Answer $\frac{\mu_0 I}{\sqrt{2} R}$ at an angle of $45^{\circ}$ with either of the two fields 📝
Detailed Solution

Since the coils are identical and carry the same current $I$, the magnitude of the magnetic field produced by each coil at their common centre is equal:

$$B_P = B_Q = B = \frac{\mu_0 I}{2R}$$

The coils are in perpendicular planes, so their respective magnetic fields at the centre are also perpendicular to each other ($\vec{B_P} \perp \vec{B_Q}$).

The magnitude of the net magnetic field ($B_{net}$) is the vector sum of these two perpendicular fields:

$$B_{net} = \sqrt{B_P^2 + B_Q^2} = \sqrt{B^2 + B^2} = \sqrt{2B^2} = \sqrt{2} B$$
$$B_{net} = \sqrt{2} \left( \frac{\mu_0 I}{2R} \right) = \frac{\mu_0 I}{\sqrt{2} R}$$

The direction of the net magnetic field relative to the field of coil P is given by:

$$\tan \theta = \frac{B_Q}{B_P} = \frac{B}{B} = 1 \implies \theta = 45^\circ$$

Thus, the net magnetic field acts at an angle of $45^\circ$ with respect to the magnetic field of either coil.

Related Posts


Also check

Class-wise Contents


Leave a Reply

Join Telegram Channel

Editable Study Materials for Your Institute - CBSE, ICSE, State Boards (Maharashtra & Karnataka), JEE, NEET, FOUNDATION, OLYMPIADS, PPTs

Discover more from Gurukul of Excellence

Subscribe now to keep reading and get access to the full archive.

Continue reading