Force on a Moving Charge (OCR A Level Physics): Revision Note

Exam code: H556

Katie M

Written by: Katie M

Reviewed by: Caroline Carroll

Updated on

Force on a Moving Charge

  • The magnetic force on an isolated moving charged particle, such as a proton, is given by the equation:

F = BQv

  • Where:

    • F = magnetic force on the particle (N)

    • B = magnetic flux density (T)

    • Q = charge of the particle (C)

    • v = speed of the particle (m s−1)

  • This is the maximum force on the charged particle, when F, B and v are mutually perpendicular

    • Therefore if a particle travels parallel to a magnetic field, it will not experience a magnetic force

 

  • Current is the rate of flow of positive charge

    • This means that the direction of the 'current' for a flow of negative charge (e.g. an electron beam) is in the opposite direction to its motion

  • If the charged particle is moving at an angle θ to the magnetic field lines, then the size of the magnetic force F is given by the equation: 

F = BQv sin θ

  • This equation shows that: 

    • The size of the magnetic force is zero if the angle θ is zero (i.e. the particle moves parallel to the field lines)

    • The size of the magnetic force is maximum if the angle θ is 90° (i.e. the particle moves perpendicular to field lines)

Worked Example

A beta particle is incident at 70° to a magnetic field of flux density 0.5 mT, travelling at a speed of 1.5 × 106 m s–1.

Calculate: 

a) The magnitude of the magnetic force on the beta particle

b) The magnitude of the maximum possible force on a beta particle in this magnetic field, travelling with the same speed

Answer:

Part (a)

Step 1: Write out the known quantities

  • Magnetic flux density B = 0.5 mT = 0.5 × 10−3 T

  • Speed v = 1.5 × 106 m s–1

  • Angle θ between the flux and the velocity = 70°

Step 2: Substitute quantities into the equation for magnetic force on a charged particle

  • A beta particle is an electron

  • Therefore, the magnitude of electron charge Q = 1.6 × 10–19 C

  • Substituting values gives:

BQv sin θ

F = (0.5 × 10–3) × (1.6 × 10–19) × (1.5 × 106) × sin (70)

F = 1.1 × 10–16 N

Part (b)

Step 1: Write out the known quantities

  • Magnetic flux density B = 0.5 mT = 0.5 × 10–3 T

  • Speed v = 1.5 × 106 m s–1

Step 2: Determine the angle to the flux lines

  • Angle θ between the flux and the velocity = 90° if the magnetic force is a maximum

Step 3: Substitute quantities into the equation for magnetic force on a charged particle

  • The magnitude of electron charge Q = 1.6 × 10–19 C

    • Substituting values gives:

BQv sin θ BQv when sin 90 = 1

F = (0.5 × 10–3) × (1.6 × 10–19) × (1.5 × 106)

F = 1.2 × 10–16 N

Examiner Tips and Tricks

Remember not to mix this up with F = BIL sin θ!

  • F = BIL sin θ is the force on a current-carrying conductor

  • F = BQv sin θ is the force on an isolated moving charged particle (which may be inside a conductor)

Another super important fact to remember for typical exam questions is that the magnetic force on a charged particle is centripetal, because it always acts at 90° to the particle's velocity. You should practise using Fleming's Left Hand Rule to determine the exact direction! 

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Katie M

Author: Katie M

Expertise: Curriculum Expert

Katie has always been passionate about the sciences, and completed a degree in Astrophysics at Sheffield University. She decided that she wanted to inspire other young people, so moved to Bristol to complete a PGCE in Secondary Science. She particularly loves creating fun and absorbing materials to help students achieve their exam potential.

Caroline Carroll

Reviewer: Caroline Carroll

Expertise: Head of Content Delivery

Caroline graduated from the University of Nottingham with a degree in Chemistry and Molecular Physics. She spent several years working as an Industrial Chemist in the automotive industry before retraining to teach. Caroline has over 12 years of experience teaching GCSE and A-level chemistry and physics. She is passionate about delivering high-quality resources to help students achieve their full potential.