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Motion of Charged Particles in a Uniform Magnetic Field

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Estimated time: 8 minutes
CISCE: Class 12

Introduction

When a charged particle moves through a uniform magnetic field, it experiences a magnetic (Lorentz) force that is always perpendicular to its velocity. This force does no work on the particle — it changes only the direction of motion, never the speed.

Think of a ball tied to a string and whirled in a circle. The string always pulls the ball toward the centre (never speeds it up or slows it down) — exactly how the magnetic force acts on a charged particle. This is why circular/helical paths, not straight-line acceleration, result.

CISCE: Class 12

Magnetic Force on a Moving Charge

A charge q moving with velocity v at an angle θ to a uniform field B experiences a force:

F = qv B sin⁡ θ

This is the magnitude form of the Lorentz force law, \[\vec F\] = q(\[\vec v\] × \[\vec B\]).

CISCE: Class 12

Case 1 — Velocity Parallel to Field

Velocity Parallel to Field (θ = 0° or 180°)

  • F = qv B sin⁡(0°) = 0
  • No magnetic force acts on the particle.
  • Result: The particle continues in a straight line, undeviated, at constant speed.

CISCE: Class 12

Case 2 — Velocity Perpendicular to Field

Velocity Perpendicular to Field (θ = 90°)

  • F = qvB acts as the centripetal force.
  • The particle moves in a uniform circular path in the plane perpendicular to B.

Charge sign effect:

  • Positive charge → curves one way (say, clockwise, per right-hand rule).
  • Negative charge → curves the opposite way (anticlockwise).

Radius in terms of other quantities:

  • r = \[\frac{mv}{qB}=\frac{p}{qB}=\frac{\sqrt{2mK}}{qB}=\frac{1}{B}\sqrt{\frac{2mV}{q}}\]

where p = momentum, K = kinetic energy, V = accelerating potential.

CISCE: Class 12

Case 3 — Velocity at an Angle θ to Field

Velocity at an Angle θ to Field (Oblique Entry)

  • Velocity is resolved into two components:
    Parallel: v = v cos ⁡θ → produces uniform straight-line motion along B
    Perpendicular: v = v sin⁡ θ → produces circular motion
  • Combined effect: the particle traces a helical path along the direction of B.

CISCE: Class 12

Real-Life Applications

  • Cyclotron: Uses the circular motion of charged particles in a magnetic field to accelerate them to high energies.
  • Mass Spectrometer: Uses the radius formula r = \[\frac {mv}{qB}\]​ to separate ions by mass-to-charge ratio.
  • Van Allen Belts: Charged particles from solar wind spiral helically along Earth's magnetic field lines — a real-world helical motion example.
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