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Magnetic Effects of Current

Pick Biot–Savart (local source) or Ampere (symmetry), get B, then apply F=q v×B or F=I ℓ×B; meter problems are shunt/series multiplier arithmetic.

Portion ElectromagnetismFocus Biot–Savart/Ampere fields, forces and meter conversions — high Advanced densityTarget 60–90sPortion share 9.8%Trend Rising
Syllabus centres on straight wire, circular coil axis and long solenoid, plus force on charges/wires, loop magnetic moment and galvanometer→ammeter/voltmeter conversions. Magnetic template: source of B → symmetry → F or τ via cross product → energy only from electric or changing flux elsewhere.

How Advanced asks this

  • B on axis of loop / due to wire / inside solenoid
  • Force or torque on a current loop or wire in B
  • Path of charged particle in uniform B (radius, pitch)
  • Ammeter/voltmeter conversion resistances
  • Statement audits on Ampere applicability

Traps that leak marks

  • Using centre-of-loop B formula on the axis far away
  • Applying Ampere to a finite wire as if infinite
  • Forgetting sinθ in F=IℓB sinθ
  • Swapping shunt and series multiplier
  • Claiming magnetic force changes speed (it only bends path when F⊥v)
  • Claiming magnetic force changes kinetic energy
  • Using Ampère’s easy B without symmetry
  • Forgetting sinθ in |v×B| or |L×B|

01. Biot–Savart builds B from current elements; Ampere’s law ∮B·dl=μ₀ I_enc is the symmetry shortcut (infinite straight wire, long solenoid, etc.).

02. Straight long wire: B=μ₀ I/(2π r). Coil axis: B=μ₀ I R²/2(R²+x²)^{3/2}. Long solenoid: B=μ₀ n I inside (ideal).

03. Force: F=q(v×B) on charges; F=I(ℓ×B) on wires. Parallel currents attract if same direction.

04. Loop moment m=IA; τ=m×B, U=−m·B in uniform B. Galvanometer conversions: shunt for ammeter, series multiplier for voltmeter.

05. Magnetic force on a charge is q(v×B); on a wire Idl×B. Force does no work on a charged particle—speed stays constant in pure B; only direction changes.

06. Biot–Savart and Ampère need symmetry honesty (straight wire, loop, solenoid, sheet). Right-hand rules are orientation tools, not substitutes for vector products.

07. Torque on a dipole m×B; energy −m·B in uniform B. Moving charges in crossed E and B: cyclotron ω=qB/m; drift when E and B are perpendicular.

Official · 2026

Syllabus for this topic

Official syllabus points for Magnetic Effects of Current only — not the full Electromagnetism portion map. Portion hub: Electromagnetism · Magnetism/EMI/AC analysis.

Syllabus on this page is topic-scoped: Magnetic Effects of Current. The parent portion (Magnetism/EMI/AC) also covers other topics — use the portion hub for the full map.

Must cover (this topic)

  • Biot–Savart / Ampere field formulae

Gaps / watch-outs

No topic-specific exclusions flagged — finish the unit points below for Magnetism.

Source: https://jeeadv.ac.in/documents/jee-advanced-2026-syllabus.pdf

Unit 01

Magnetic Effects of Current

high

Exam focusBiot–Savart/Ampere fields, Lorentz force, and current-carrying geometry.

Syllabus points

  • Biot–Savart and Ampere; field of straight wire, circular coil axis, long solenoid
  • Force on moving charge and current wire; magnetic moment of loop; galvanometer/voltmeter/ammeter conversions

Full Physics syllabus →

Cross-topic stems

Mixed joins for this topic

Advanced rarely asks a chapter in isolation. These are tagged multi-idea Physics stems that touch Magnetic Effects of Current — practise the knowledge bridge, not only the single-chapter drill.

No tagged mixed stem matched this topic’s keywords yet. Still revise the joins listed under Trends, and scan the mixed joins board for Mechanics / EM / Optics bridges.

All mixed joins →

Why methods matter

Common methods that change your score

Right-hand directions plus Ampere/Biot choice organise magnetic field and force asks.

01

Ampere symmetry gate

Stops fake ∮B·dl = B·2πr on asymmetric currents.

Do thisUse Ampere only when |B| is constant on the Amperian path by symmetry.

Why it works

Stops fake ∮B·dl = B·2πr on asymmetric currents.

See it once

Infinite straight wire: circle centred on wire → B·2πr = μ₀ I.

02

Right-hand direction lock

Force direction errors dominate wrong options.

Do thisDetermine B direction before magnitude; mark × / · on the figure.

Why it works

Force direction errors dominate wrong options.

See it once

Thumb along I, fingers curl in B for a loop; F uses v×B separately.

03

Uniform-B loop split

Prevents claiming translation from uniform B alone.

Do thisNet F=0 on closed loop in uniform B; keep τ=m×B.

Why it works

Prevents claiming translation from uniform B alone.

See it once

Only nonuniform B yields net force on a magnetic dipole.

04

Meter partition

One current-split picture covers both conversions.

Do thisGalvanometer full-scale I_g through G; excess current through shunt, excess voltage on series R.

Why it works

One current-split picture covers both conversions.

See it once

Ammeter: I_g G = (I−I_g) R_s; voltmeter: I_g(G+R)=V.

Processed examples

Sample questions · full working

Read the impact line first. Then notice which family/model was chosen. The solution is written the way your rough sheet should look in the hall.

01

bankFamily · Biot–Savart / Ampere field

Sample question

Find B at distance a from a long straight wire carrying I.

This stem rewards early recognition of the biot–savart / ampere field model.

Model chosenAmpere: B·2πa=μ₀I.

Processed solution

  1. B=μ₀I/(2πa).

Answerμ₀I/(2πa)

Takeaway: High symmetry ⇒ Ampere’s law.

02

standardFamily · Lorentz force on charge/wire

Sample question

A proton moves at 10⁶ m/s perpendicular to B=0.1 T. Find the magnetic force. Take e=1.6×10⁻¹⁹ C.

This stem rewards early recognition of the lorentz force on charge/wire model.

Model chosenF=qvB.

Processed solution

  1. F=1.6×10⁻¹⁴ N.

Answer1.6×10⁻¹⁴ N

Takeaway: Maximum force when v⊥B.

03

twistFamily · Lorentz force on charge/wire

Sample question

A particle with charge q and mass m enters a region of uniform B=Bẑ with velocity v₀î. A uniform electric field E=Eĵ is also present. Find E so that the particle goes undeflected, and the pitch if instead E=0 and a small v_z is added.

This Advanced-level variation couples hidden constraints with the lorentz force on charge/wire model.

Model chosenUndeflected ⇒ E+v×B=0; helical pitch uses parallel velocity.

Processed solution

  1. For undeflected straight motion, E=−v×B ⇒ E=−v₀ B ĵ? v×B=v₀ B ĵ, so E=−v₀B ĵ cancels.
  2. Magnitude E=v₀B.
  3. If E=0 and v=v_⊥î+v_z k̂, cyclotron ω=qB/m and pitch = v_z T=2πm v_z/(qB).

AnswerE=v₀B (opposite v×B); pitch=2πm v_z/(qB)

Takeaway: Crossed E×B selects a speed; parallel v makes helices.

Reusable models

Common question families

Advanced stems cluster. Name the family in 10–15s, write the fast model, then run the same path. Do not invent a new plan each time.

01

Biot–Savart / Ampere field

Looks likeWire, loop axis, solenoid, or sheet

Fast modelUse Ampere when symmetry is high; Biot–Savart for finite pieces.

Same solve path

  1. Choose Biot–Savart or Ampere.
  2. Write B magnitude and direction (right-hand).
  3. Superpose contributions.
  4. Evaluate on axis or mid-plane as asked.

Rough skeleton

  • law choice
  • B vector
  • superpose

Why faster

Recognition fixes the model before arithmetic begins.

Refuse this

Do not start blind expansion or casework before identifying the governing model.

02

Lorentz force on charge/wire

Looks likeF=q(v×B) or Iℓ×B; cyclotron radius

Fast modelKeep vector directions; r=mv/(qB) for ⊥ motion.

Same solve path

  1. Write velocity and B directions.
  2. Compute F direction and magnitude.
  3. For circles, use centripetal = qvB.
  4. Include E if crossed fields.

Rough skeleton

  • v,B
  • F
  • orbit

Why faster

Recognition fixes the model before arithmetic begins.

Refuse this

Do not start blind expansion or casework before identifying the governing model.

03

Magnetic moment and torque

Looks likeLoop μ=IA; τ=μ×B; U=−μ·B

Fast modelFind area vector; then μ and torque/energy.

Same solve path

  1. Find I and area vector.
  2. Form μ.
  3. Apply τ and U in uniform B.
  4. For coils, multiply by turns.

Rough skeleton

  • μ
  • τ/U
  • result

Why faster

Recognition fixes the model before arithmetic begins.

Refuse this

Do not start blind expansion or casework before identifying the governing model.

04

Force between current elements

Looks likeParallel wires attraction/repulsion

Fast modelF/L = μ₀ I₁ I₂ /(2πd); same direction attracts.

Same solve path

  1. Identify current directions.
  2. Write F/L formula.
  3. Integrate finite length if needed.
  4. State attract/repel.

Rough skeleton

  • directions
  • F/L
  • net F

Why faster

Recognition fixes the model before arithmetic begins.

Refuse this

Do not start blind expansion or casework before identifying the governing model.

Hall timing

60–90s process

  1. 0–15s
    Classify: find B, find force/torque, particle motion, or meter conversion.

    Underline charges, geometry, symmetry, source type and the exact ask (E, V, flux, I, B, Φ, energy). Reject any formula whose assumptions are already broken.

  2. 15–35s
    Choose Biot–Savart formula or Ampere symmetry; fix right-hand direction.

    Write the governing law symbolically before numbers: Coulomb/Gauss, Kirchhoff, Biot–Savart/Ampere, Faraday/Lenz, or phasor impedance. Fix sign convention and reference once.

  3. 35–75s
    Compute B then F/τ/path, or R_shunt/R_series from Ig and G.

    Compute with ratios and conserved quantities first. Carry direction, SI units and powers of ten on the rough sheet instead of repairing them at the end.

  4. 75–90s
    Check μ₀ factors, direction (attract/repel), and that uniform-B loop force nets to zero.

    Check dimensions, limiting cases (κ→1, r→∞, ω→0/∞) and physical sense. For multi-correct, test every option independently.

After the model is locked

Quick formula bank

Biot–Savart (wire)

dB = (μ₀/4π) I dl×r̂ / r²

General current element

Long straight wire

B = μ₀ I/(2π r)

Infinite straight current

Loop centre / axis

B_centre=μ₀ I/(2R); axis B=μ₀ I R²/2(R²+x²)^{3/2}

Circular coil

Long solenoid

B = μ₀ n I (inside, ideal)

Dense long solenoid

Lorentz / wire force

F=q v×B; F=I ℓ×B

Force on charge or straight segment

Cyclotron radius

r = mv/(qB) (v⊥); T=2πm/(qB)

Uniform B, no E

Magnetic moment

m = I A; τ = m×B; U=−m·B

Planar loop in uniform B

Ammeter shunt

R_s = I_g G / (I − I_g)

Convert G to ammeter range I

Voltmeter multiplier

R = V/I_g − G

Convert G to voltmeter range V

Mental bank

  • μ₀/4π = 10⁻⁷ T m/A
  • Wire B∝I/r; solenoid B∝nI
  • F=q v×B; magnetic force ⊥ v
  • Parallel currents: same direction attract
  • m=IA; τ=mB sinθ
  • Ammeter: shunt parallel; voltmeter: series R
  • Uniform B: net F on closed loop = 0
  • F=q(v×B); no magnetic work on q
  • F=I L×B for straight wire in uniform B
  • τ=m×B; U=−m·B (uniform)
  • ω_c=qB/m for cyclotron motion

Make it automatic

Practice · checklist

Daily

  • Three B calculations (wire, axis, solenoid) and one meter conversion.
  • One charged-particle radius/pitch mental numerical.

Weekly

  • Force/torque mixed sheet with direction marking.
  • Statement drill: Ampere applicability and uniform-B loop force.

100% checklist

  • Biot–Savart vs Ampere chosen correctly
  • Direction fixed with right-hand rule
  • Correct catalogue formula for geometry
  • F or τ used with proper vector angle
  • Meter formulas matched ammeter/voltmeter
  • μ₀ and powers of ten checked
  • Uniform vs nonuniform B distinguished for net force
  • Vector product directions fixed with a sketch
  • Symmetry checked before Ampère/Biot shortcuts
  • Work/energy: magnetic force does no work on free q