CBSE Class 12 Physics Chapter 7: Moving Charges and Magnetism NCERT Solutions

NCERT Solutions PDF Class 12 PDF

This resource provides comprehensive NCERT Solutions for CBSE Class 12 Physics, Chapter 7, focusing on Moving Charges and Magnetism. It covers additional exercises, offering detailed step-by-step explanations for calculating magnetic fields produced by current-carrying coils and designing solenoids. The solutions clarify the application of fundamental formulas, vector nature of magnetic fields, and practical considerations in electromagnetism. These solutions are designed to help students grasp complex concepts, reinforce their understanding of electromagnetic principles, and prepare effectively for their board examinations by providing clear, accurate, and easy-to-follow problem-solving strategies.

Quick info

BoardCBSE
ClassClass 12
SubjectPhysics
Session2026
LanguageEnglish
TypeNCERT Solutions
ChapterChapter 7

Chapter summary

This chapter's NCERT Solutions for Class 12 Physics delve into the principles of moving charges and magnetism. The provided solutions focus on additional exercises, detailing the calculation of magnetic fields at the center of concentric circular coils and exploring the design parameters for a solenoid to achieve a specific magnetic field strength. Students will find clear explanations of the formulas governing magnetic fields and their directions, aiding in the practical application of these concepts.

Learning outcomes

  • Calculate the net magnetic field at the center of concentric circular coils.
  • Determine the direction of the magnetic field using the right-hand rule.
  • Apply the formula for the magnetic field inside a solenoid.
  • Suggest design parameters for a solenoid based on required magnetic field strength and material constraints.
  • Understand the relationship between current, turns, radius, and magnetic field.
  • Convert magnetic field units (Gauss to Tesla).

Topics covered

Paper topics

  • Magnetic field at the center of a circular coil
  • Direction of magnetic field (Right-hand rule)
  • Net magnetic field from multiple coils
  • Magnetic field inside a solenoid
  • Design parameters of a solenoid
  • Unit conversion (Gauss to Tesla)

Important topics

  • Magnetic field calculation for circular coils
  • Determining magnetic field direction
  • Solenoid magnetic field formula
  • Solenoid design considerations

PDF preview

Read page by page below. PDF is streamed from the official NCERT website — no download button on this page.

Loading document …
Page of
Loading page …

Questions and Solutions

Question 4.14

Two concentric circular coils X and Y of radii 16 cm and 10 cm, respectively, lie in the same vertical plane containing the north to south direction. Coil X has 20 turns and carries a current of 16 A; coil Y has 25 turns and carries a current of 18 A. The sense of the current in X is anticlockwise, and clockwise in Y, for an observer looking at the coils facing west. Give the magnitude and direction of the net magnetic field due to the coils at their centre.
Solution:

We are given the following information:

  • Radius of coil X, r_1 = 16 \text{ cm} = 0.16 \text{ m}
  • Radius of coil Y, r_2 = 10 \text{ cm} = 0.10 \text{ m}
  • Number of turns in coil X, N_1 = 20
  • Number of turns in coil Y, N_2 = 25
  • Current in coil X, I_1 = 16 \text{ A}
  • Current in coil Y, I_2 = 18 \text{ A}
  • Permeability of free space, \mu_0 = 4\pi \times 10^{-7} \text{ T m A}^{-1}

The magnetic field at the center of a circular coil is given by the formula B = \frac{\mu_0 N I}{2r}.

For coil X, the current is anticlockwise when viewed from the west. Using the right-hand rule, this current produces a magnetic field directed towards the East at the center.

The magnitude of the magnetic field due to coil X is:

B_1 = \frac{\mu_0 N_1 I_1}{2r_1} = \frac{(4\pi \times 10^{-7} \text{ T m A}^{-1}) \times 20 \times 16 \text{ A}}{2 \times 0.16 \text{ m}}

B_1 = \frac{4\pi \times 10^{-7} \times 320}{0.32} = 4\pi \times 10^{-4} \text{ T (Towards East)}

For coil Y, the current is clockwise when viewed from the west. Using the right-hand rule, this current produces a magnetic field directed towards the West at the center.

The magnitude of the magnetic field due to coil Y is:

B_2 = \frac{\mu_0 N_2 I_2}{2r_2} = \frac{(4\pi \times 10^{-7} \text{ T m A}^{-1}) \times 25 \times 18 \text{ A}}{2 \times 0.10 \text{ m}}

B_2 = \frac{4\pi \times 10^{-7} \times 450}{0.20} = 9\pi \times 10^{-4} \text{ T (Towards West)}

Since the magnetic fields B_1 and B_2 are in opposite directions (East and West), the net magnetic field at the center is the difference between their magnitudes. The direction of the net field will be the same as the direction of the larger field.

Net magnetic field, B = |B_2 - B_1|

B = |9\pi \times 10^{-4} \text{ T} - 4\pi \times 10^{-4} \text{ T}| = 5\pi \times 10^{-4} \text{ T}

Substituting the value of \pi \approx 3.14:

B = 5 \times 3.14 \times 10^{-4} \text{ T} = 15.7 \times 10^{-4} \text{ T} = 1.57 \times 10^{-3} \text{ T}

Since B_2 (towards West) is greater than B_1 (towards East), the net magnetic field is directed towards the West.

Answer: The magnitude of the net magnetic field at the centre is 1.57 \times 10^{-3} \text{ T} and its direction is towards the West.

Question 4.15

A magnetic field of 100 G (1 G = 10^{-4} T) is required which is uniform in a region of linear dimension about 10 cm and area of cross-section about 10^{-3} m2. The maximum current carrying capacity of a given coil of wire is 15 A and the number of turns per unit length that can be wound round a core is at most 1000 turns m-1. Suggest some appropriate design particulars of a solenoid for the required purpose. Assume the core is not ferromagnetic.
Solution:

We need to design a solenoid that produces a uniform magnetic field of 100 G in a specific region. The given parameters are:

  • Required magnetic field strength, B = 100 \text{ G} = 100 \times 10^{-4} \text{ T} = 10^{-2} \text{ T}
  • Maximum number of turns per unit length, n_{max} = 1000 \text{ turns m}^{-1}
  • Maximum current carrying capacity, I_{max} = 15 \text{ A}
  • Permeability of free space, \mu_0 = 4\pi \times 10^{-7} \text{ T m A}^{-1}

The magnetic field inside a long solenoid is given by the formula B = \mu_0 n I. We need to find values of n and I such that B = 10^{-2} \text{ T}, and n \le n_{max} and I \le I_{max}.

Let's consider the maximum possible turns per unit length, n = 1000 \text{ turns m}^{-1}. We can then calculate the required current I using the formula:

I = \frac{B}{\mu_0 n} = \frac{10^{-2} \text{ T}}{(4\pi \times 10^{-7} \text{ T m A}^{-1}) \times (1000 \text{ turns m}^{-1})}

I = \frac{10^{-2}}{4\pi \times 10^{-4}} \text{ A} = \frac{100}{4\pi} \text{ A} = \frac{25}{\pi} \text{ A}

Calculating the value of \frac{25}{\pi}:

I \approx \frac{25}{3.14} \text{ A} \approx 7.96 \text{ A}

Since the required current I \approx 7.96 \text{ A} is less than the maximum allowed current I_{max} = 15 \text{ A}, this design is feasible.

Therefore, appropriate design particulars for the solenoid are:

  • Number of turns per unit length, n = 1000 \text{ turns m}^{-1}
  • Current, I \approx 7.96 \text{ A}

The solenoid should be wound to have 1000 turns per meter and operated with a current of approximately 7.96 A to produce a magnetic field of 100 G. The length of the solenoid should be chosen such that it provides a uniform field over the required region of 10 cm linear dimension. For a long solenoid, the field is uniform in the central region.

Common mistakes

  • Incorrectly applying the right-hand rule to determine the direction of the magnetic field.
  • Errors in unit conversions (e.g., cm to m, Gauss to Tesla).
  • Calculation mistakes when dealing with multiple coils or complex solenoid parameters.
  • Confusing the formulas for magnetic fields from different current configurations.

Revision tips

  • Review the right-hand rule for determining magnetic field direction for both coils and solenoids.
  • Practice unit conversions carefully before solving problems.
  • Ensure you understand the formula for magnetic field at the center of a circular coil and inside a solenoid.
  • Work through the design problem for the solenoid to understand the interplay of different parameters.

Practice MCQs

Q1. What is the direction of the magnetic field at the center of a circular coil when the current flows counter-clockwise?

Q2. If two coils are concentric and carry currents in opposite senses, how is the net magnetic field at the center determined?

Q3. What is the unit of magnetic field strength in the SI system?

Q4. For a solenoid, the magnetic field strength is directly proportional to:

Frequently asked questions

What is the formula for the magnetic field at the center of a circular coil?

The magnetic field (B) at the center of a circular coil with N turns, carrying current I and having radius r is given by B = (μ₀NI) / (2r).

How do you determine the direction of the magnetic field produced by a circular coil?

The direction can be found using the right-hand rule: curl the fingers of your right hand in the direction of the current in the coil; your thumb points in the direction of the magnetic field at the center.

What is the magnetic field inside a long solenoid?

The magnetic field inside a long solenoid is uniform and is given by B = μ₀nI, where n is the number of turns per unit length and I is the current.

How can we find the net magnetic field when two coils are present?

The net magnetic field is the vector sum of the individual magnetic fields. If the fields are in opposite directions, you subtract their magnitudes; if in the same direction, you add them.

What are the key parameters to consider when designing a solenoid for a specific magnetic field?

Key parameters include the number of turns per unit length (n), the current (I), the radius of the solenoid, and the permeability of the core material. The required magnetic field strength (B) dictates the combination of these parameters.

Content reviewed by the NCERT Help team. Editorial Team and update policy

NCERT Solutions PDF PDF on NCERT Help. URL unchanged for search indexing.