Lorentz Force on a Moving Charge
Lorentz force is the total force on a charge q moving with velocity v in the presence of electric field E and magnetic field B, given by F = q(E + v x B).
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Student-friendly explanation
The electric part qE acts whether the charge is moving or at rest. The magnetic part q(v x B) acts only when the charge has velocity with a component perpendicular to the magnetic field. Its direction is perpendicular to both v and B, and it is reversed for a negative charge. If v is perpendicular to B and there is no electric field, the magnetic force provides centripetal force, so the charge moves in a circular path.
How to write this in exams
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Start with the exact idea
Lorentz force is the total force on a charge q moving with velocity v in the presence of electric field E and magnetic field B, given by F = q(E + v x B).
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Then show how to use it
Identify q, m, v, B, and angle theta. Choose F = qvB sin theta for magnetic force. For circular motion with perpendicular entry, equate qvB to mv^2/r. Substitute SI units. Decide force direction using v x B and reverse it for a negative charge.
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Add one concrete example
An electron entering a uniform magnetic field at right angles follows a circular path. The magnetic force changes the direction of velocity but not the speed because it is always perpendicular to the motion.
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Avoid this incomplete answer
Using r = qB/(mv) reverses the formula and gives a physically wrong result, where faster particles would have smaller radius.
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Quick check
Why does a charged particle moving perpendicular to a uniform magnetic field move in a circular path?
It moves in a circular path because the magnetic force qvB is always perpendicular to its velocity and acts as the centripetal force. The force changes only the direction of motion, not the speed.
Answer writing and exam use
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