Common misconceptions

Common mistake
Wrong: A charged particle moving parallel to a magnetic field experiences a maximum magnetic force.
Right: A charged particle moving parallel to a magnetic field experiences zero magnetic force because F = qvB sinθ and sin(0°) = 0.
The sinθ term in F = qvB sinθ is the key — when velocity is parallel to the magnetic field, θ = 0°, and sin(0°) = 0, so the force is exactly zero. The magnetic force only exists when there's a component of velocity perpendicular to the field. Maximum force occurs at θ = 90°, when the charge moves perpendicular to B.
Common mistake
Wrong: The magnetic force does work on a moving charge, changing its speed as it curves.
Right: The magnetic force is always perpendicular to velocity, so it does no work and changes direction but not speed; the particle moves in a circle at constant speed.
The magnetic force is always perpendicular to the velocity vector, which means it can never do work on the charge (since W = F·d requires a force component along displacement). No work means no change in kinetic energy, so speed stays constant. The force only redirects the particle — it continuously changes direction without speeding it up or slowing it down, producing uniform circular motion.
Common mistake
Gap: Fails to reverse the right-hand rule result for negative charges when finding magnetic force direction
The right-hand rule for F = qv × B requires pointing fingers in the direction of v, curling toward B, with the thumb giving the force direction for positive charges; for negative charges, the force is reversed.
The right-hand rule gives you the direction of F for a positive charge. For negative charges, the force is in the exact opposite direction — so after applying the right-hand rule, flip it 180°. A common fix: point fingers along v, curl toward B, thumb points toward F for positive charges; if the charge is negative, the actual force is opposite your thumb. Always check the sign of q before finalizing your answer.
Common mistake
Wrong: In a mass spectrometer, ions with greater mass travel in a smaller radius arc.
Right: In a mass spectrometer, r = mv/qB, so heavier ions (larger m) travel in a larger radius arc, allowing mass separation.
From r = mv/qB, radius is directly proportional to mass — double the mass, double the radius. Heavier ions curve less sharply and land farther from the source, which is exactly how a mass spectrometer separates ions by mass. The intuition that heavier things get deflected more (smaller radius) applies to gravity, not magnetic deflection — don't cross-wire those models.
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What the exam tests

  1. Know the Lorentz force law F = qvB sinθ — including what the angle θ refers to and how to use the right-hand rule to find the direction of force on a moving charge.
  2. Explain why a charged particle in a uniform magnetic field travels in a circle at constant speed, and use r = mv/qB to predict how changing mass, charge, velocity, or field strength affects the radius.
  3. Calculate the magnetic force on a moving charge or current-carrying wire given numerical values of charge, velocity, field strength, and angle.
  4. Apply magnetic force principles to real-world contexts like mass spectrometry (mass separation by arc radius), cyclotrons (repeated acceleration), and MRI (proton alignment and precession).

Can you avoid these mistakes?

A proton moves due east in a magnetic field pointing due north. Using the right-hand rule, in which direction does the magnetic force act? Now repeat for an electron moving in the same direction through the same field.
Two ions with the same charge and velocity enter a uniform magnetic field perpendicular to their motion. Ion A has twice the mass of Ion B. Which one traces the larger circular arc, and by how much?
A charged particle enters a region of uniform magnetic field and moves in a perfect circle. Its speed is measured at two points on the circle and found to be identical. A classmate says the magnetic force must be doing work to keep it moving. What's wrong with that reasoning?
In a mass spectrometer, singly ionized carbon-12 and carbon-14 atoms are accelerated through the same voltage and enter the same magnetic field perpendicular to their motion. Which isotope hits the detector farther from the entry point, and what does that tell you about how the device separates isotopes?

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