You are currently viewing Motion in a Magnetic Field: Circles and Helixes
JEE Main and Advanced5 min readSep 4, 2026Updated Sep 5, 2026

Motion in a Magnetic Field: Circles and Helixes

Motion in a Magnetic Field: Circles and Helixes
5 min read · 950 words

JEE/NEET Physics · Moving Charges & Magnetism series · Part 2 of 8 · All parts →

✪ Key points — the 30-second version

  • Charge moving ⊥ to B: uniform circular motion — B supplies the centripetal force
  • Radius: r = mv/(qB) — fast or heavy means wide; strong field or big charge means tight
  • Period: T = 2πm/(qB) — independent of SPEED (the cyclotron’s secret)
  • Velocity with a component along B: helix (circle + slide)
  • Work done by B is always zero: speed never changes

Fire a charge across a magnetic field and it can’t escape — the sideways force bends it into a perfect circle. The field is the ultimate invisible roundabout, and the radius of the circle tells you the particle’s momentum. Part 2 of the Moving Charges & Magnetism series.

In this card

  1. The magnetic roundabout
  2. Radius and period
  3. Speed-blind timing
  4. The helix
  5. Solved examples
  6. Common mistakes
  7. This physics in your daily life
  8. Practice set
  9. Recap

The Magnetic Roundabout

Magnetic force ⊥ velocity is exactly the job description of centripetal force (the Circular Motion card): set qvB = mv²/r and the circle appears by itself. Unlike friction or gravity, the field never tires and never changes the speed — steering only, forever.

Radius and Period

r = mv/(qB) · T = 2πm/(qB)r carries momentum information; T is fixed by the field alone
LetterWhat it means (plain words)Value / unit
rorbit radiusm
Tperiod of one laps — no v inside!
m, qparticle’s mass and chargekg, C

Speed-Blind Timing

The miracle: fast particles travel bigger circles in the SAME time — T depends only on m, q, B. A slow particle’s small circle and a fast one’s big circle complete together, like runners on concentric tracks finishing in a tie.

The Helix

Velocity partly along B: the parallel component slides freely (no force along B), the perpendicular part circles — the path is a helix, a spiral around the field line. This is how charged particles spiral along Earth’s field lines to the poles.

Solved Examples

✎ Easy — the radius. Electron at 10⁶ m/s ⊥ to 0.01 T field. r? (m = 9.1×10⁻³¹)

r = mv/qB = (9.1×10⁻³¹ × 10⁶)/(1.6×10⁻¹⁹ × 0.01) ≈ 5.7×10⁻⁴ m — about half a millimetre.

Answer: ≈0.57 mm

✎ Exam level — the period. Same electron: time per lap?

T = 2πm/(qB) = 2π(9.1×10⁻³¹)/(1.6×10⁻¹⁹ × 0.01) ≈ 3.6 ns — a billion laps per second-ish.

Answer: ≈3.6 ns

✎ JEE level — separating isotopes. U²³⁸⁺ and U²³⁵⁺ (same speed, same B) enter a mass spectrometer. Radius ratio?

r ∝ m (same q, v): r₂₃₈/r₂₃₅ = 238/235 ≈ 1.013 — a 2 mm separation on a 15 cm track.

Enough to separate uranium isotopes: the Manhattan Project’s calutrons were this exact card.

Answer: 238 : 235

⚠ Mistakes students make — and how to avoid them

  • Changing speed inside B. Never — magnetic forces steer only; if speed changes, something electric is also present.
  • Period depending on v. It doesn’t — T = 2πm/qB: fast particles simply ride wider circles.
  • Helix forgotten for angled entry. Component along B slides unchecked — the particle escapes along the field line while circling.
  • Using the wrong m for electrons vs protons. Same formula, 1836× different mass: radii and periods differ correspondingly.

This Physics in Your Daily Life

◎ This physics in your daily life

  • Mass spectrometers — r = mv/qB separates molecules by mass: drug tests, forensics, and doping labs all measure circle sizes.
  • Van Allen belts — charged particles helixing along Earth’s field lines: radiation belts discovered by this geometry.
  • Auroras spiral along field lines to the poles — the helix in action at planetary scale, glowing where they meet the atmosphere.
  • Cyclotrons in hospitals — proton therapy beams circle up to cancer-killing energies: r = mv/qB written into medical hardware.
  • Bubble chambers of particle physics history — trails of tiny circles, each radius a particle’s identity card: discovery by curvature.
One idea, three doors — open whichever clicks for you
Same concept (why circles, and why speed-blind timing), three different ways of seeing it. If one door confuses you, try the next — at least one will stick.
Door 1 · The story way

Tie a ball to a string and swing: the string’s inward pull makes a circle. A magnetic field is an invisible string that never shortens, never snaps, never lets go — and never changes the speed. The result can only be perfect uniform circular motion.

Door 2 · The numbers way

Double the speed: the circle doubles its radius, but the lap time (2πm/qB) hasn’t changed — the fast particle’s longer path exactly cancels its speed. Triple it: same again. It’s the only force law with this property, and it’s why cyclotrons work at all.

Door 3 · The picture way

Draw velocity arrows around a circle, each ⊥ to its radius, with the magnetic force arrow repeatedly turning the velocity’s tip: the arrows trace the circle like a compass drawing it. Add a slide-along-B arrow and the drawing becomes a spring-shape: the helix.

Why is this happening at all? Why does the period come out speed-blind? Algebra: T = 2πr/v = 2π(mv/qB)/v — the v’s cancel identically. Physics: faster particles travel proportionally bigger circles. Why circles at all? Because a force that stays perpendicular to a fixed-speed velocity is the textbook definition of circular motion — circular motion card meets the magnetic field and they fit perfectly.

Practice set (answers hidden — try first)

(NEET-level) Doubling v in fixed B: r
Doubles.
(JEE Main-level) Doubling B at fixed v: r
Halves.
(NEET-level) T depends on:
m, q, B only — not v.
(Concept) Charge with velocity component along B moves in a
Helix.
(JEE Main-level) Proton vs electron, same v, B: r_p/r_e =
1836 (mass ratio).
🧠 Memory tricks & everyday anchors — the 20-second revision

  • qvB = mv²/r → circles
  • r = mv/(qB) — a momentum meter
  • T = 2πm/(qB), speed-independent
  • angled entry → helix
  • speed never changes in B alone
  • 🔁 circular motion condition
  • 🔁 radius and period formulas
  • 🔁 speed independence
▶ Recap card — save for revision week

  • 🧠 Chant: ‘fast rides wide, arrives on time’.
  • 🧠 Radius reads momentum — mass spectrometry in one line.
  • 🏠 Daily: auroras spiral on field lines.
  • 🏠 Daily: hospital cyclotrons circle protons to therapy energy.

Quick revision

  • Charge moving ⊥ to B: uniform circular motion — B supplies the centripetal force
  • Radius: r = mv/(qB) — fast or heavy means wide; strong field or big charge means tight
  • Period: T = 2πm/(qB) — independent of SPEED (the cyclotron’s secret)
  • Velocity with a component along B: helix (circle + slide)
  • Work done by B is always zero: speed never changes
  • This physics in your daily life
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