Moving Charges and Magnetism
NCERT Class 12 Physics Chapter 4
Moving Charges and Magnetism for Class 12 Physics, JEE and NEET: Lorentz force, Biot–Savart and Ampere’s laws, solenoids and the moving coil galvanometer.
10 topics Updated 8 Nov 2026
For: Class 12, JEE and NEET, unless a topic says otherwise
In the syllabus: JEE Class 12 syllabus, NEET Class 12 syllabus
With your textbook
NCERT Physics Part I (Class 12), Chapter 4 “Moving Charges and Magnetism”, reprint 2026-27.
Open the official NCERT chapter (PDF, 3.7 MB, ncert.nic.in) (opens in a new tab)
Checked on 19 Oct 2026.
Learn in this order
-
Magnetic force and the Lorentz force
F = q(E + v × B), magnetic force |q|vB sin θ, directions, the tesla and force on a wire, with examples.
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Motion of a charge in a magnetic field
Why a charge circles, r = mv/(qB), frequency qB/(2πm), helical paths and the pitch, with examples.
-
Biot–Savart law: the field of a current element
The statement and vector form, dB = μI dl sin θ/(4πr), direction of dB, μ and Coulomb’s law, with examples.
-
Magnetic field on the axis of a circular current loop
Formula and derivation, μI/(2R) at the centre, arcs, N turns and direction.
-
Ampere’s circuital law
Statement and sign rule, amperian loops, B = μI/(2πr) for a long wire, B inside a thick wire, examples.
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The solenoid
B = μnI from Ampere’s law, uniform inside and nearly zero outside, direction, ends, examples.
-
Force between two parallel currents and the ampere
Derivation of the force per metre, why like currents attract, and the ampere’s definition.
-
Torque on a current loop and the magnetic dipole
Derivation of τ = IAB sin θ, magnetic moment m = NIA, τ = m × B, and the loop as a magnetic dipole.
-
The moving coil galvanometer
The radial field, φ = (NAB/k)I, conversion to an ammeter and a voltmeter, and its sensitivity.
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Experiment: resistance and figure of merit of a galvanometer
The half-deflection method, G = RS/(R − S), k = ε/[(R + G)θ], precautions, examples.
Key formulas in this chapter
Magnetic force
- F = q(E + v × B)
- F = |q|vB sin θ
- F = I l × B
- F = IlB sin θ
- 1 T = 1 N s C m = 10 G
Motion in a magnetic field
- r = mv/(qB)
- ω = 2πν = qB/m
- T = 2πm/(qB)
- pitch: p = 2πm v cos θ/(qB)
- r = √(2mK)/(qB)
Biot–Savart law
- vector form: dB = (μ/4π) I dl × r/r
- dB = μ I dl sin θ/(4πr)
- μ/4π ≈ 10 T m/A
- εμ = 1/c
- dB = 0 along the line of the element
Field on the axis of a loop
- B = μ0 I R2/[2(x2 + R2)3/2]
- B0 = μ0 I/(2R)
- N turns: B = μNI/(2R)
- arc of angle φ: B = μIφ/(4πR)
- far on the axis: B ≈ μIR/(2x)
Ampere’s circuital law
- ∮ B · dl = μI
- BL = μ0 Ie
- B = μI/(2πr)
- inside a uniform wire: B = μIr/(2πa)
- B ∝ r inside, ∝ 1/r outside
The solenoid
- B = μnI
- n = N/l
- Bh = μI(nh)
- at an end: B ≈ μnI/2
- outside a long solenoid: B ≈ 0
Force between parallel currents
- F = μ0 Ia Ib L/(2πd)
- f = μ0 Ia Ib/(2πd)
- Fba = −Fab
- 1 A, 1 m apart: f = 2 × 10 N/m
- same direction attract, opposite repel
Torque on a current loop
- τ = IAB sin θ
- m = NIA
- τ = m × B
- U = −m · B
- far on the axis: B = (μ/4π)(2m/x)
Moving coil galvanometer
- kφ = NIAB
- φ/I = NAB/k
- φ/V = NAB/(kRG)
- shunt: rs = Ig RG/(I − Ig)
- voltmeter: R = V/Ig − RG
Experiment: galvanometer resistance
- G = RS/(R − S) ≈ S (R ≫ S)
- k = ε/[(R + G)θ]
- current sensitivity = 1/k
- I1 = ε/(R + G)
- full scale: Ig = k × divisions
More in Physics
- Units and Measurement
- Motion in a Straight Line
- Motion in a Plane
- Laws of Motion
- Work, Energy and Power
- Systems of Particles and Rotational Motion
- Gravitation
- Mechanical Properties of Solids
- Mechanical Properties of Fluids
- Thermal Properties of Matter
- Thermodynamics
- Kinetic Theory
- Oscillations
- Waves
- Electric Charges and Fields
- Electrostatic Potential and Capacitance
- Current Electricity
- Magnetism and Matter
- Electromagnetic Induction
- Alternating Current
- Electromagnetic Waves
- Ray Optics and Optical Instruments
- Wave Optics
- Dual Nature of Radiation and Matter
- Atoms
- Nuclei
- Semiconductor Electronics: Materials, Devices and Simple Circuits