CBSE Class 12 Physics Chapter 4 Moving Charges and Magnetism NCERT Solutions

NCERT Solutions PDF Class 12 PDF

This comprehensive set of NCERT Solutions for CBSE Class 12 Physics, Chapter 4, "Moving Charges and Magnetism," delves into the fundamental principles governing the interaction between moving charges and magnetic fields. The solutions cover key concepts such as the Biot-Savart Law, the Lorentz force, the motion of charged particles in uniform magnetic fields (including helical paths), and the working principles of devices like the cyclotron. Detailed explanations are provided for multiple-choice questions, helping students grasp the underlying physics. These solutions are designed to aid students in understanding complex topics, reinforcing their knowledge, and preparing effectively for their board examinations by offering clear, step-by-step problem-solving approaches.

Quick info

BoardCBSE
ClassClass 12
SubjectPhysics Exemplar
Session2026
LanguageEnglish
TypeNCERT Solutions
ChapterChapter 4

Chapter summary

Chapter 4 of the CBSE Class 12 Physics syllabus, "Moving Charges and Magnetism," explores the magnetic effects of electric currents. This section provides NCERT Solutions that clarify concepts like the magnetic field produced by moving charges, the Biot-Savart Law, the force on a current-carrying conductor in a magnetic field, and the motion of charged particles in magnetic fields. The solutions focus on understanding the direction and magnitude of magnetic fields and forces, and the principles behind devices like cyclotrons.

Learning outcomes

  • Understand the relationship between moving charges and magnetic fields.
  • Apply the Biot-Savart Law to calculate magnetic fields.
  • Analyze the motion of charged particles in uniform magnetic fields.
  • Explain the working principle of a cyclotron.
  • Solve problems involving magnetic forces on moving charges.

Topics covered

Paper topics

  • Magnetic Field due to a Current Element (Biot-Savart Law)
  • Force on a Moving Charge in a Magnetic Field (Lorentz Force)
  • Motion of Charged Particles in Uniform Magnetic Fields
  • Helical Path of Charged Particles
  • Cyclotron
  • Magnetic Moment of a Current Loop
  • Magnetic Field due to a Straight Wire
  • Magnetic Field due to a Solenoid

Important topics

  • Lorentz Force
  • Motion in a Uniform Magnetic Field
  • Biot-Savart Law
  • Cyclotron Principle
  • Magnetic Moment

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Questions and Solutions

Multiple Choice Questions (MCQs) - Q. 1

Two charged particles traverse identical helical paths in a completely opposite sense in a uniform magnetic field $\mathbf{B} = \mathbf{B}_0 \hat{\mathbf{k}}$.

(a) They have equal z-components of momenta

(b) They must have equal charges

(c) They necessarily represent a particle, anti-particle pair

(d) The charge to mass ratio satisfy $\left(\frac{e}{m}\right)_1 + \left(\frac{e}{m}\right)_2 = 0$

Solution: The helical path of a charged particle in a uniform magnetic field is characterized by its radius and pitch. The radius depends on the component of velocity perpendicular to the field and the charge-to-mass ratio ($r = mv_{\perp}/(qB)$), while the pitch depends on the component of velocity parallel to the field and the charge-to-mass ratio ($Pitch = 2\pi mv_{\parallel}/(qB)$). Since the particles traverse identical helical paths but in opposite senses, their pitches must be the same, and the radii must be the same. For the paths to be in opposite senses, the charges must have opposite signs, while maintaining the same magnitude of charge-to-mass ratio. Therefore, if $q_1/m_1$ and $q_2/m_2$ are the charge-to-mass ratios, we must have $q_1/m_1 = -q_2/m_2$. This implies $\left(\frac{q}{m}\right)_1 + \left(\frac{q}{m}\right)_2 = 0$. Considering $e$ as charge, the condition is $\left(\frac{e}{m}\right)_1 + \left(\frac{e}{m}\right)_2 = 0$.

Answer: (d)

Multiple Choice Questions (MCQs) - Q. 2

Biot-Savart law indicates that the moving electrons (velocity $\nu$) produce a magnetic field $\mathbf{B}$ such that

(a) B is perpendicular of

(b) B is parallel to v

(c) it obeys inverse cube law

(d) it is along the line joining the electron and point of observation

Solution: The Biot-Savart law describes the magnetic field $d\mathbf{B}$ generated by a small current element $I d\mathbf{l}$ as $d\mathbf{B} = \frac{\mu_0}{4\pi} \frac{I d\mathbf{l} \times \mathbf{r}}{r^3}$, where $\mathbf{r}$ is the position vector from the element to the point of observation. For a moving electron, the current element $I d\mathbf{l}$ is in the direction opposite to the electron's velocity $\mathbf{v}$. The direction of $d\mathbf{B}$ is given by the cross product $d\mathbf{l} \times \mathbf{r}$. This cross product is always perpendicular to both $d\mathbf{l}$ (and thus to $\mathbf{v}$) and $\mathbf{r}$. Therefore, the magnetic field $\mathbf{B}$ is perpendicular to the velocity $\mathbf{v}$ of the electron.

Answer: (a)

Multiple Choice Questions (MCQs) - Q. 3

A current carrying circular loop of radius R is placed in the x-y plane with centre at the origin. Half of the loop with $x > 0$ is now bent so that it now lies in the y-z plane.

(a) The magnitude of magnetic moment now diminishes

(b) The magnetic moment does not change

(c) The magnitude of B at $(0,0,z)$, $z > R$, increases

(d) The magnitude of B at $(0,0,z)$, $z \gg R$, is unchanged

Solution: The magnetic moment $\mathbf{M}$ of a current loop is given by $M = IA$, where $I$ is the current and $A$ is the area vector (magnitude $A = \pi R^2$ and direction perpendicular to the plane of the loop). Initially, the circular loop of radius R is in the x-y plane, so its magnetic moment $\mathbf{M}_{initial} = I(\pi R^2) \hat{\mathbf{k}}$. When half of the loop (where $x > 0$) is bent to lie in the y-z plane, the original loop is effectively replaced by two semi-circular loops. The semi-circular part remaining in the x-y plane (where $y > 0$) has a magnetic moment $\mathbf{M}_1 = I(\pi R^2/2) \hat{\mathbf{k}}$. The bent semi-circular part (where $x > 0$ originally, now in y-z plane) has its area vector pointing along the x-axis, so its magnetic moment is $\mathbf{M}_2 = I(\pi R^2/2) \hat{\mathbf{i}}$. The new net magnetic moment is the vector sum: $\mathbf{M}_{net} = \mathbf{M}_1 + \mathbf{M}_2 = I(\pi R^2/2) \hat{\mathbf{k}} + I(\pi R^2/2) \hat{\mathbf{i}}$. The magnitude of the net magnetic moment is $M_{net} = \left|\mathbf{M}_{net}\right| = \sqrt{\left(I\frac{\pi R^2}{2}\right)^2 + \left(I\frac{\pi R^2}{2}\right)^2} = \sqrt{2 \left(I\frac{\pi R^2}{2}\right)^2} = \frac{I \pi R^2}{\sqrt{2}}$. Comparing the initial magnitude $M_{initial} = I \pi R^2$ with the net magnitude $M_{net} = \frac{I \pi R^2}{\sqrt{2}}$, we see that $M_{net} < M_{initial}$. Therefore, the magnitude of the magnetic moment diminishes.

Answer: (a)

Multiple Choice Questions (MCQs) - Q. 4

An electron is projected with uniform velocity along the axis of a current carrying long solenoid. Which of the following is true?

(a) The electron will be accelerated along the axis

(b) The electron path will be circular about the axis

(c) The electron will experience a force at 45° to the axis and hence execute a helical path

(d) The electron will continue to move with uniform velocity along the axis of the solenoid

Solution: A long solenoid carrying current produces a magnetic field that is predominantly uniform and directed along its axis. When an electron is projected with a uniform velocity along this axis, its velocity vector $\mathbf{v}$ is parallel to the magnetic field vector $\mathbf{B}$. The magnetic Lorentz force acting on a charged particle is given by $\mathbf{F} = q(\mathbf{v} \times \mathbf{B})$. Since $\mathbf{v}$ is parallel to $\mathbf{B}$, the angle $\theta$ between them is $0^\circ$. The magnitude of the cross product $\mathbf{v} \times \mathbf{B}$ is $vB \sin \theta = vB \sin 0^\circ = 0$. Therefore, the magnetic force on the electron is zero ($\mathbf{F} = 0$). As there is no force acting on the electron, it will continue to move with its initial uniform velocity along the axis of the solenoid.

Answer: (d)

Multiple Choice Questions (MCQs) - Q. 5

In a cyclotron, a charged particle

(a) undergoes acceleration all the time

(b) speeds up between the dees because of the magnetic field

(c) speeds up in a dee

(d) slows down within a dee and speeds up between dees

Solution: A cyclotron uses both electric and magnetic fields to accelerate charged particles. The magnetic field is uniform and perpendicular to the plane of the dees, causing the charged particle to move in a circular path within each dee. This magnetic field only changes the direction of the velocity, not its magnitude. The electric field is applied across the gap between the dees. Each time the particle crosses this gap, it is accelerated by the electric field, gaining kinetic energy and increasing its speed. This acceleration happens repeatedly as the particle spirals outwards. Therefore, the charged particle undergoes acceleration and speeds up every time it crosses the gap between the dees.

Answer: (a)

Common mistakes

  • Confusing the direction of magnetic fields and forces.
  • Incorrectly applying the Lorentz force formula.
  • Misinterpreting the conditions for helical motion.
  • Errors in calculating magnetic moments of current loops.

Revision tips

  • Review the Biot-Savart Law and its applications thoroughly.
  • Practice problems involving the Lorentz force and circular/helical motion.
  • Understand the vector nature of magnetic fields and forces.
  • Visualize the paths of charged particles in magnetic fields.
  • Focus on the conditions under which forces are zero or maximum.

Practice MCQs

Q1. Two charged particles traverse identical helical paths in a uniform magnetic field $\mathbf{B} = \mathbf{B}_0 \hat{\mathbf{k}}$ but in opposite senses. Which of the following conditions must be satisfied?

Q2. According to the Biot-Savart law, the magnetic field $\mathbf{B}$ produced by a moving electron with velocity $\nu$ is such that:

Q3. A current-carrying circular loop of radius R in the x-y plane is partially bent such that its right half (x > 0) now lies in the y-z plane. How does the magnetic moment change?

Q4. An electron moves with uniform velocity along the axis of a current-carrying long solenoid. What happens to the electron?

Q5. In a cyclotron, a charged particle:

Frequently asked questions

What is the main topic of CBSE Class 12 Physics Chapter 4?

Chapter 4, "Moving Charges and Magnetism," focuses on the magnetic effects produced by moving electric charges and currents, and the forces experienced by charges and currents in magnetic fields.

How does the Biot-Savart law help in understanding magnetic fields?

The Biot-Savart law allows us to calculate the magnetic field generated by a small segment of a current-carrying wire. It's fundamental for determining magnetic fields from various current configurations.

What is the Lorentz force?

The Lorentz force is the total force experienced by a charged particle moving in an electromagnetic field. It has two components: the electric force and the magnetic force ($F = qE + q(v \times B)$).

Under what conditions does a charged particle move in a helical path in a magnetic field?

A charged particle moves in a helical path when its velocity has components both parallel and perpendicular to a uniform magnetic field. The perpendicular component causes circular motion, while the parallel component causes uniform linear motion along the field lines.

How can these NCERT Solutions help in exam preparation?

These solutions provide clear, step-by-step explanations for complex problems, helping students understand the concepts, practice problem-solving techniques, and identify common mistakes, thereby boosting their confidence for exams.

What is the role of a cyclotron?

A cyclotron is a particle accelerator that uses a magnetic field to bend the path of charged particles and an electric field to accelerate them, allowing them to gain high energies.

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