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.
Topic match inside parent portion Magnetism/EMI/AC (9.8% of Physics tags). Stats below are portion backdrop; matched subtopics show where Magnetic Effects of Current sits.
Portion share9.8%
TrendRising
Study intensityRotate · fortnightly
Avg / year3.29
This topic in papers
Magnetism — 11 tagged (47.8% of Magnetism/EMI/AC)20:121:322:123:124:326:2
Portion-wide type/difficulty mix lives on the Magnetism/EMI/AC analysis — not repeated here so this page stays on Magnetism.
01. Magnetism/EMI/AC accounts for ~9.8% of tagged physics questions (2020–2026).
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.
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
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
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
For undeflected straight motion, E=−v×B ⇒ E=−v₀ B ĵ? v×B=v₀ B ĵ, so E=−v₀B ĵ cancels.
Magnitude E=v₀B.
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
Choose Biot–Savart or Ampere.
Write B magnitude and direction (right-hand).
Superpose contributions.
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
Write velocity and B directions.
Compute F direction and magnitude.
For circles, use centripetal = qvB.
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
Find I and area vector.
Form μ.
Apply τ and U in uniform B.
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
Identify current directions.
Write F/L formula.
Integrate finite length if needed.
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
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.
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.
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.
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