Overview
This lesson explains the Hall effect and how Hall probes measure magnetic flux density. You will
connect magnetic force on charge carriers to a measurable transverse voltage.
What You Need to Know
- Moving charge carriers in a magnetic field experience a sideways magnetic force.
- Charge builds up on opposite sides of the conductor until the electric force balances the magnetic
force.
- This separation produces a Hall voltage.
- The Hall voltage is given by VH = BI / (ntq), where n is number density, t is thickness, and q is
the charge of each carrier.
- A Hall probe uses a calibrated Hall voltage to measure magnetic flux density.
How to Work Through It
- Draw the conductor, current direction, magnetic field, and sideways force.
- Explain how charge separation creates an opposing electric field.
- Use the balanced-force derivation to reach VH = BI / (ntq).
- Practise using the equation and interpreting Hall probe readings.
Check Your Understanding
- Why does the Hall voltage stop increasing once equilibrium is reached?
- How does increasing current affect Hall voltage?
- Why are semiconductors useful in Hall probes?
- What happens to the sign of the Hall voltage if the charge carriers change sign?
Common Mistakes
- Confusing conductor thickness t with the length of the sample.
- Treating number density n as the number of charge carriers rather than carriers per unit volume.
- Forgetting that the Hall voltage is across the sample, not along the current direction.
- Ignoring the sign of the charge carrier when reasoning about polarity.
Next Steps
- Use Hall probe ideas to interpret magnetic field measurements in later induction work.
- Keep the moving-charge force model secure.