Complete NEET prep for Magnetism and Matter: bar magnet, magnetic dipole moment, field on axis and equator, torque, Earth's magnetism, magnetic intensity, susceptibility, diamagnetic / paramagnetic / ferromagnetic substances, hysteresis. NCERT-aligned notes, 30+ PYQs and live interactive widgets. Built for NEET 2027.
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NEET Questions
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A bar magnet behaves like a magnetic dipole with moment m = pole strength times length
Field of a bar magnet on the axis (2 k m / r cubed) and on the equator (k m / r cubed)
Torque on a bar magnet in a uniform B: tau = m B sin theta
Earth's magnetic field: declination, dip, horizontal and vertical components
Magnetic intensity H, magnetisation M, susceptibility chi, relative permeability mu_r
Diamagnetic (chi small negative), paramagnetic (chi small positive), ferromagnetic (chi very large)
Curie's law: M proportional to H over T for paramagnets
Hysteresis loop, retentivity and coercivity for ferromagnets
Five worked NEET problems on every type of question
20 questions from Magnetism and Matter across the last 5 NEET papers.
NEET 2024
4
questions
NEET 2023
4
questions
NEET 2022
4
questions
NEET 2021
4
questions
NEET 2020
4
questions
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You can expect 1 question from this chapter in NEET 2027. The chapter has medium PYQ frequency. Bar magnet field and torque, Curie's law, classification of magnetic materials and basics of Earth's magnetism are favourites.
A bar magnet with pole strength m_pole and length 2 L has dipole moment vector p_m equals m_pole times 2 L, directed from south to north pole. Unit: A m squared (or J per T). For a current loop of N turns, area A and current I, the moment is m equals N I A.
On the axis at distance r far from the magnet, B equals 2 mu_0 m over (4 pi r cubed). On the equator (perpendicular bisector), B equals mu_0 m over (4 pi r cubed). Axial is twice equatorial. Both fall as 1 over r cubed.
Three numbers describe Earth's field at any place: declination (angle between true geographic north and magnetic north on a map), dip or inclination (angle B makes with the horizontal plane), and horizontal component B_H. Total field B equals B_H over cos(dip).
Diamagnetic: weakly repelled by a magnet. chi is small and NEGATIVE (around -10⁻⁵). Examples: bismuth, copper, water. Paramagnetic: weakly attracted. chi is small and POSITIVE (around +10⁻⁴). Examples: aluminium, oxygen. Ferromagnetic: strongly attracted, can be permanently magnetised. chi is large positive (10² to 10⁵). Examples: iron, nickel, cobalt.
For a paramagnetic substance, the magnetisation M is proportional to the applied field H and inversely proportional to absolute temperature T: M equals C H over T, where C is the Curie constant. Equivalently, susceptibility chi equals C over T. Heating reduces magnetisation.
For a ferromagnetic material, the M vs H curve traces a loop instead of a straight line. Starting from zero, M rises with H to saturation. When H is reversed, M does not retrace the same path: there is residual magnetism (retentivity) at H equals 0, and M only reaches zero at a reverse field called the coercivity. The area of the loop equals the energy lost per cycle as heat.
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