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Force on a Moving Charge (CIE A Level Physics)

Revision Note

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Calculating magnetic force on a moving charge

  • A moving charge produces its own magnetic field
    • When interacting with an applied magnetic field, it will experience a force
  • The force F on an isolated particle with charge Q moving with speed v at an angle θ to a magnetic field with flux density B is defined by the equation

F space equals space B Q v space sin space theta

  • 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)
    • θ = angle between charge’s velocity and magnetic field (degrees)
  • Current is taken as the rate of flow of positive charge (i.e. conventional current)
    • This means that the direction of the current for a flow of negative charge (e.g. a beam of electrons) is in the opposite direction to its motion
  • As with a current-carrying conductor, the maximum force on a charged particle occurs when it travels perpendicular to the field
    • This is when θ = 90°, so sin θ = 1
  • The equation for the magnetic force becomes:

F space equals space B Q v

  • F, B and v are mutually perpendicular, therefore:
    • if the direction of the particle's motion changes, the magnitude of the force will also change
    • if the particle travels parallel to a magnetic field, it will experience no magnetic force

Path of a moving charged particle in a magnetic field

Force on isolated moving charge, downloadable AS & A Level Physics revision notes

The force on an isolated moving charge is perpendicular to its motion and the magnetic field B

  • From the diagram above, when a beam of electrons enters a magnetic field which is directed into the page: 
    • electrons are negatively charged, so current I is directed to the right (as motion v is directed to the left)
    • using Fleming’s left-hand rule, the force on an electron will be directed upwards

Direction of force on a moving charge

  • The direction of the magnetic force on a charged particle depends on
    • the direction of flow of the current
    • the direction of the magnetic field
  • This can be found using Fleming's left-hand rule
  • The second finger represents the current flow or the flow of positive charge
    • For a positive charge, the current points in the same direction as its velocity 
    • For a negative charge, the current points in the opposite direction to its velocity

7-8-4-flemings-left-hand-rule-charged-particles

Fleming’s left-hand rule allows us to determine the direction of the force on a charged particle

  • From the diagram above, when a positive charge enters a magnetic field from left to right, using Fleming's left-hand rule:
    • the first finger (field) points into the page
    • the second finger (current) points to the right
    • the thumb (force) points upwards
  • When a charged particle moves in a uniform magnetic field, the force acts perpendicular to the field and the particle's velocity
    • As a result, it follows a circular path 

Direction of Magnetic Force, downloadable AS & A Level Physics revision notes

The direction of the magnetic force F on positive and negative particles in a B field in and out of the page

Worked example

An electron moves in a uniform magnetic field of flux density 0.2 T at a velocity of 5.3 × 107 m s−1.

Calculate the force on the electron when it moves perpendicular to the field.

Answer:

Step 1: Write out the known quantities

  • Velocity of the electron, v = 5.3 × 107 m s−1
  • Charge of an electron, Q = 1.60 × 10−19 C
  • Magnetic flux density, B = 0.2 T

Step 2: Write down the equation for the magnetic force on an isolated particle

F space equals space B Q v space sin space theta

  • The electron moves perpendicular (θ = 90°) to the field, so sin θ = 1

F space equals space B Q v

Step 3: Substitute in values, and calculate the force on the electron

F = (0.2) × (1.60 × 10−19) × (5.3 × 107) = 1.7 × 10−12 N (2 s.f.)

Examiner Tip

Remember not to mix this up with F = BIL!

  • F = BIL is for a current carrying conductor
  • F = BQv is for an isolated moving charge (which may be inside a conductor)

Remember not to get this mixed up with Fleming's right-hand rule. That is used for a generator (or dynamo), where a current is induced in the conductor. Fleming's left-hand rule is sometimes referred to as the 'Fleming's left-hand rule for motors'.

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Ashika

Author: Ashika

Expertise: Physics Project Lead

Ashika graduated with a first-class Physics degree from Manchester University and, having worked as a software engineer, focused on Physics education, creating engaging content to help students across all levels. Now an experienced GCSE and A Level Physics and Maths tutor, Ashika helps to grow and improve our Physics resources.