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