Magnetism and Matter Class 12 Physics Formula Sheet 2026-27 | Important Formulas
Magnetism and Matter Class 12 Physics — Formula Sheet + Quick Revision
A compact, syllabus-aware Magnetism and Matter Class 12 Physics formula sheet covering important formulas, magnetic dipole moment, torque, magnetic field lines, magnetic materials, magnetisation, magnetic susceptibility, permeability and exam traps for quick revision.
For 2026–27, use the first three relationships as the core revision anchors; susceptibility/permeability are retained as conceptual relationships supported by CBSE learning outcomes.
1. Magnetic Dipole Moment
Current-carrying coil
m = magnetic dipole moment, N = number of turns, I = current, A = area of the coil. SI unit: A m².
Direction of magnetic moment
Use the right-hand rule: curl fingers in the direction of current; the thumb gives the direction of m.
2. Torque on a Magnetic Dipole
Magnitude of torque
θ is the angle between magnetic dipole moment m and magnetic field B. The torque tends to rotate the dipole toward alignment with the field.
θ = 90° → τmax = mB
θ = 0° or 180° → τ = 0
3. Magnetic Field of a Bar-Magnet Dipole — Current-Syllabus View
| Position | What to remember | Revision cue |
|---|---|---|
| Axial position | Point lies on the magnetic dipole axis. | Think “along the axis”. |
| Equatorial position | Point lies on the perpendicular bisector/equatorial line of the dipole. | Think “perpendicular to the axis”. |
| Distance dependence | The ideal dipole field decreases as distance increases; the detailed inverse-cube relation belongs here only as historical quantitative practice. | For a current-scope qualitative question, explain the trend rather than forcing a derivation. |
4. Historical Dipole-Field Relations — Use Only as Legacy PYQ Practice
Axial field of a short magnetic dipole
Historical quantitative relation. Use with the scope note above.
Equatorial field of a short magnetic dipole
Magnitude relation for the ideal short-dipole model; direction is opposite to the dipole-moment direction on the equatorial line.
5. High-Yield Extended Relations
Gauss's law for magnetism
The net magnetic flux through any closed surface is zero. This is associated with the fact that magnetic field lines form closed loops rather than beginning or ending at isolated magnetic poles.
Magnetic field in matter
B is magnetic flux density, H is magnetic intensity and M is magnetisation.
Magnetisation relation
For a linear magnetic material, magnetisation is proportional to magnetic intensity; χ is magnetic susceptibility.
Relative permeability
Useful for classification questions and directly relevant to the 2026–27 SQP's magnetic-material question.
Magnetic intensity
Rearranged from B = μ0(H + M). SI unit of H: A m⁻¹.
Permeability
Use this with the material model being assumed. μ has SI unit T m A⁻¹ (equivalently N A⁻²).
6. Magnetic Field Lines — Fast Revision
7. Dia-, Para- and Ferromagnetic Materials
| Type | Response in an external field | Susceptibility χ | Typical examples |
|---|---|---|---|
| Diamagnetic | Weakly repelled by a magnetic field. | Small and negative. | Bismuth, copper, silver, water. |
| Paramagnetic | Weakly attracted by a magnetic field. | Small and positive. | Aluminium, platinum, oxygen. |
| Ferromagnetic | Strongly attracted; can show strong magnetisation. | Large and positive in the usual simplified comparison. | Iron, cobalt, nickel. |
8. Magnetisation
Definition
M is magnetisation, i.e. magnetic dipole moment per unit volume of the material. Dimensions: magnetic moment/volume; SI unit: A m⁻¹.
SI unit
Magnetisation is measured in ampere per metre.
9. Susceptibility and Permeability — Conceptual Revision
Magnetic susceptibility
A dimensionless measure describing the magnetic response of a material to the magnetising field H. In the standard linear treatment, M = χH.
Relative permeability
Useful as a conceptual relationship in the usual linear-material treatment. Interpret it together with the material classification.
- Dia: weak repulsion, χ < 0.
- Para: weak attraction, χ small and positive.
- Ferro: strong attraction/ordering, strongly temperature-dependent.
- Magnetisation: magnetic moment per unit volume, SI unit A m⁻¹.
10. Temperature Effect on Magnetic Properties
| Material | Temperature revision idea |
|---|---|
| Paramagnetic | Magnetic response generally decreases as temperature increases; thermal agitation opposes alignment. |
| Ferromagnetic | Increasing temperature weakens ferromagnetic ordering; above the Curie temperature, the material loses ferromagnetic behaviour and becomes paramagnetic in the standard model. |
| Diamagnetic | Diamagnetic response is comparatively weak and much less temperature-sensitive in the standard school-level treatment. |
11. One-Minute Concept Map
| Concept | Remember this |
|---|---|
| Bar magnet | Model it as a magnetic dipole. |
| Equivalent solenoid | Bar magnet can be understood qualitatively as equivalent to a current-carrying solenoid. |
| Magnetic moment | For a current loop: m = NIA. |
| Torque | τ = mB sinθ; maximum at 90°, zero at 0° and 180°. |
| Field lines | Closed loops; never intersect. |
| Diamagnetic | Weak repulsion; χ is negative. |
| Paramagnetic | Weak attraction; χ is small and positive. |
| Ferromagnetic | Strong magnetic response; temperature can destroy ferromagnetic ordering. |
| Magnetisation | M = magnetic moment per unit volume; SI unit A m⁻¹. |
12. Common Exam Traps
- Trap 1: Do not confuse the direction of magnetic field lines outside a bar magnet (N → S) with the conventional direction of magnetic dipole moment (S → N).
- Trap 2: Do not call every positive-susceptibility material simply “paramagnetic”; ferromagnetic materials have a much stronger response.
- Trap 3: Diamagnetic means weakly repelled, not “completely unaffected”.
- Trap 4: Torque is zero at both θ = 0° and θ = 180°.
- Trap 5: Do not turn the current qualitative bar-magnet field treatment into an unnecessary derivation for a 2026–27 syllabus question.
- Trap 6: Unit III carries 17 marks collectively for Chapters 4 and 5; CBSE does not assign a fixed standalone 17 marks to Chapter 5.
13. 20-Minute Revision Sequence
- 2 minutes — magnetic dipole and magnetic moment.
- 3 minutes — torque and orientations.
- 4 minutes — field lines and axial/equatorial qualitative picture.
- 5 minutes — dia-, para- and ferromagnetic comparison.
- 3 minutes — magnetisation, susceptibility and temperature effect.
- 3 minutes — attempt selected Chapter 5 PYQs and check the traps above.
14. 60-Second Self-Check
- Can I state m = NIA and its SI unit?
- Can I identify when τ is maximum and zero?
- Can I distinguish axial and equatorial positions?
- Can I classify a material from the sign of χ?
- Can I explain why ferromagnetic behaviour weakens with increasing temperature?
- Can I state the current-syllabus boundary without importing obsolete quantitative requirements?
Continue Your Chapter 5 Preparation
Research note: This is an original revision resource, not an official CBSE document. The current syllabus boundary is based on the official CBSE 2026–27 Physics curriculum. Historical quantitative dipole-field relations are explicitly marked as legacy PYQ practice rather than current compulsory quantitative syllabus content.
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