Part of MAG-01 — Magnetic Effects of Current & Magnetism

Cornell Notes — Subtopic: Circular Motion of Charged Particles in Magnetic Fields

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Cue ColumnNotes Column
Why circular path?Magnetic force F = qvB is always ⊥ to v → centripetal force; no work done
Radius of circular pathr = mv/(qB); [r] = [M·LT1LT^{-1} / A·T·MT^{-2}$$A^{-1}] = [L] = m
Time periodT = 2πm/(qB); depends only on m, q, B — NOT on velocity or radius
Cyclotron frequencyf = qB/(2πm); used in cyclotron particle accelerators
Helical path conditionComponent v_∥ along B → no force; component v_⊥ to B → circular; net = helix
Pitch of helixp = v_∥ × T = v cosθ × (2πm/qB)
Proton vs alpha in same fieldr_p = m_pv/(eB); r_α = 4m_pv/(2eB) = 2r_p; alpha has twice the radius
Velocity selectorWhen qE = qvB: v = E/B; selects particles of specific speed

Summary: A charge moving perpendicular to B traces a perfect circle (no work done by B). The cyclotron period is uniquely independent of speed — this is the key NEET insight. If velocity has a component along B, the path becomes helical. The pitch equals v_∥ × T.

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