H1 Physics 8867 · objective lesson
Force and deflection of moving charges
Use F = BQv sinθ perpendicular to motion; combine electric and magnetic forces for deflection and velocity selection.
Repair the common break
Common misconception: A magnetic field changes a charged particle’s speed.
Correct model: Use F = BQv sinθ perpendicular to motion; combine electric and magnetic forces for deflection and velocity selection.
Worked transfer
A magnetic force Qv × B is perpendicular to velocity, so it changes direction but does no work. In crossed fields, undeflected motion requires qE and qvB to oppose, giving v = E/B.
Guided practice
Explain why “A magnetic field changes a charged particle’s speed.” fails. Then construct one example that correctly applies force and deflection of moving charges.
Independent practice
A proton enters crossed fields E = 3.0 × 10⁴ V m⁻¹ and B = 0.20 T. Find the undeflected speed and state how an electron at that speed behaves.
Return to the recorded repair plan when the explanation and application are secure enough to re-test.