You are currently viewing Magnetism Finale: The Formula Card and the Motor Age
JEE Main and Advanced4 min readSep 4, 2026Updated Sep 5, 2026

Magnetism Finale: The Formula Card and the Motor Age

Magnetism Finale: The Formula Card and the Motor Age
4 min read · 650 words

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

✪ Key points — the 30-second version

  • Eight parts on one card — force, motion, selectors, fields, laws, meters
  • F = qvB sinθ · r = mv/qB · T = 2πm/qB · v = E/B
  • Biot-Savart wire: μ₀I/2πr · solenoid: μ₀nI · Ampere: ∮B·dl = μ₀I
  • Wire force: BIl · pair: μ₀I₁I₂/2πd · torque: NIAB sinθ
  • Right-hand rules everywhere: force, grip, and circulation

The final card of the Moving Charges & Magnetism series — eight parts on one revision sheet, plus the century of machines this chapter unleashed.

In this card

  1. The master formula card
  2. The one-rule-per-part recap
  3. The motor age
  4. Final practice set
  5. Recap

The Master Formula Card

WhatFormulaRemember
Charge forceF = qvB sinθ⊥ always, no work
Radiusr = mv/(qB)momentum meter
PeriodT = 2πm/(qB)speed-blind
Velocity selectorv = E/Bone speed passes
Cyclotron fqB/(2πm)fixed tune
Wire fieldB = μ₀I/(2πr)grip rule circles
Loop centreμ₀NI/(2R)concentrator
Solenoidμ₀nIn per metre
Ampere’s law∮B·dl = μ₀I_enccount piercings
Wire forceF = BIl sinθparade pushed
Wire pairμ₀I₁I₂/(2πd)same = attract
Loop torqueNIAB sinθmotor twist
Galvanometerφ ∝ Ispring balance

The One-Rule-Per-Part Recap

1: sideways-only force on movers. 2: circles, radius = momentum. 3: crossed fields gate one speed; cyclotrons climb by fixed tune. 4: currents weave circling fields. 5: circulation counts enclosed current. 6: wires feel each other’s weavings. 7: loops twist, springs measure.

The Motor Age

◎ This physics in your daily life

  • From Oersted’s compass twitch (1820) to Faraday’s motor (1821) took ONE YEAR — this chapter’s discovery-to-machine speed remains physics’ fastest.
  • The electrified twentieth century — motors in factories, trams in cities, pumps in fields: τ = NIAB turned electrical science into mechanical civilisation.
  • Medical and research frontiers — MRI magnets, cyclotron therapy, particle colliders: Part 2 and 3 geometry saving lives and probing matter.
  • Sensors everywhere — Hall probes, clamp meters, GFCI protectors: Amperean bookkeeping embedded in daily safety.
  • Coming full circle to relativity — the tiny force between wires that Einstein couldn’t reconcile with Galilean physics opened the door to special relativity: this chapter asked the question that reshaped all of physics.
One idea, three doors — open whichever clicks for you
Same concept (why this chapter motorised the world), three different ways of seeing it. If one door confuses you, try the next — at least one will stick.
Door 1 · The story way

Electricity could only light and heat until it learned to TURN. Magnetism supplied the twist: a force that is always sideways is exactly what rotation needs. The day physics combined current loops with magnetic fields, wheels could be driven without steam — factories moved from rivers to sockets.

Door 2 · The numbers way

One loop: milli-newton-metres of torque. One hundred turns and 50 cm² later: newton-metres. Multiply by engineering decades: locomotive traction motors deliver mega-newton forces — the same NIAB sinθ, scaled by geometry and persistence.

Door 3 · The picture way

See the chapter as one machine blueprint: current source (Battery series), field weaver (Biot-Savart/Ampere), force producer (qvB/BIl), rotor (loop torque), controller (commutator), measurement (galvanometer) — every part a wall in the house the motor built.

Why is this happening at all? Why did magnetism unlock rotation when electricity alone couldn’t? Because electric force pushes along field lines — through the loop, not around it. Only the magnetic force’s sideways geometry supplies the tangential push rotation demands. Nature offered exactly one force with the right handedness — and the industrial world took it.

Practice set (answers hidden — try first)

(NEET-level) 1 μC at 10⁵ m/s ⊥ 0.4 T: F =
4×10⁻⁶×0.4… = 4×10⁻⁵ N.
(JEE Main-level) r for a proton (v=10⁷, B=0.5):
(1.67×10⁻²⁷×10⁷)/(1.6×10⁻¹⁹×0.5) ≈ 0.21 m.
(NEET-level) 3 m wire, 2 A, ⊥ 0.25 T: F =
1.5 N.
(JEE Main-level) Same-direction parallel currents:
Attract.
(NEET-level) Solenoid B with n=1000/m, I=1 A ≈
4π×10⁻⁷×1000 ≈ 1.26 mT.
🧠 Memory tricks & everyday anchors — the 20-second revision

  • F = qvB sinθ and F = BIl
  • circles: r = mv/qB, T = 2πm/qB
  • fields: wire, loop, solenoid, Ampere
  • pair force and loop torque
  • meters by shunt and multiplier
  • 🔁 the 13-row master card
  • 🔁 one rule per part
  • 🔁 motor-age perspective
▶ Recap card — save for revision week

  • 🧠 Full-card chant: ‘steer, circle, gate, weave, count, push, twist’.
  • 🏠 Daily: every motor is NIAB sinθ at work.
  • 🏠 Daily: this chapter’s puzzle birthed relativity.

Quick revision

  • Eight parts on one card — force, motion, selectors, fields, laws, meters
  • F = qvB sinθ · r = mv/qB · T = 2πm/qB · v = E/B
  • Biot-Savart wire: μ₀I/2πr · solenoid: μ₀nI · Ampere: ∮B·dl = μ₀I
  • Wire force: BIl · pair: μ₀I₁I₂/2πd · torque: NIAB sinθ
  • Right-hand rules everywhere: force, grip, and circulation
  • The one-rule-per-part recap
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