Topics
Electrostatics
Electric Charges and Fields
- Electric Charge
- Conductors and Insulators
- Properties of Electric Charge
- Coulomb’s Law
- Forces between Multiple Charges
- Electric Field
- Electric Field Due to a System of Charges
- Physical Significance of Electric Field
- Electric Field Lines
- Electric Flux
- Electric Dipole
- Dipole in a Uniform External Field
- Continuous Charge Distribution
- Gauss’s Law
- Application of Gauss' Law
Electrostatic Potential and Capacitance
- Electric Potential and Potential Energy
- Electrostatic Potential
- Electric Potential Due to a Point Charge
- Potential Due to an Electric Dipole
- Potential due to a System of Charges
- Equipotential Surfaces
- Relation Between Electric Field and Electrostatic Potential
- Potential Energy of a System of Charges
- Potential Energy of a Single Charge
- Potential Energy of a System of Two Charges in an External Field
- Potential Energy of a Dipole in an External Field
- Electrostatics of Conductors
- Dielectrics and Polarisation
- Capacitors and Capacitance
- The Parallel Plate Capacitor
- Effect of Dielectric on Capacitance
- Combination of Capacitors
- Energy Stored in a Charged Capacitor
Current Electricity
Magnetic Effects of Current and Magnetism
Current Electricity
- Electric Current
- Electric Currents in Conductors
- Ohm's Law
- Drift of Electrons and the Origin of Resistivity
- Mobility of Electrons
- Limitations of Ohm’s Law
- Resistivity of Various Materials
- Temperature Dependence of Resistivity
- Electrical Energy and Power in Conductors
- Cells, EMF, and Internal Resistance
- Cells in Series and in Parallel
- Kirchhoff’s Laws
- Wheatstone Bridge
Moving Charges and Magnetism
- Electromagnetism
- Magnetic force
- Motion in a Magnetic Field
- Magnetic Field Due to a Current-carrying Conductor: Biot-savart's Law
- Applications of Biot-Savart's Law > Magnetic Field at the Axis of a Circular Current-carrying Loop
- Ampere’s Circuital Law
- Solenoid
- Force Between Two Parallel Currents (Ampere’s Law)
- Torque on a Rectangular Current Loop in a Uniform Magnetic Field
- Circular Current Loop as a Magnetic Dipole
- Moving Coil Galvanometer
- Kirchhoff’s Laws
Electromagnetic Induction and Alternating Currents
Electromagnetic Waves
Magnetism and Matter
Electromagnetic Induction
Optics
Alternating Current
Dual Nature of Radiation and Matter
Atoms and Nuclei
Electromagnetic Waves
- Introduction to Electromagnetic Waves
- Displacement Current
- Sources of Electromagnetic Waves
- Nature of Electromagnetic Waves
- Electromagnetic Spectrum
- Definition and Characteristics of Electromagnetic Waves
Electronic Devices
Ray Optics and Optical Instruments
- Ray Optics Or Geometrical Optics
- Reflection of Light by Spherical Mirrors
- Sign Convention for Reflection by Spherical Mirrors
- Focal Length of Spherical Mirrors
- Mirror Equation of Spherical Mirrors
- Refraction of Light
- Total Internal Reflection
- Applications of Total Internal Reflection
- Refraction at a Spherical Surfaces
- Refraction by a Lens
- Power of a Lens
- Combined Focal Length of Two Thin Lenses in Contact
- Refraction Through a Prism
- Introduction to Optical Instruments
- Microscope and it’s types
- Telescope
Communication Systems
Wave Optics
- Introduction to Wave Optics
- Huygens Principle
- Refraction of a Plane Wave
- Refraction at a Rarer Medium
- Reflection of a Plane Wave by a Plane Surface
- Coherent and Incoherent Addition of Waves
- Interference of Light Waves and Young’s Experiment
- Diffraction of Light
- The Single Slit
- Seeing the Single Slit Diffraction Pattern
- Polarisation of Light
The Special Theory of Relativity
Dual Nature of Radiation and Matter
- Understanding Dual Nature of Radiation and Matter
- Electron Emission
- Photoelectric Effect - Hertz’s Observations
- Photoelectric Effect - Hallwachs’ and Lenard’s Observations
- Experimental Study of Photoelectric Effect
- Effects of Intensity and Frequency on Photocurrent
- Photoelectric Effect and Wave Theory of Light
- Einstein’s Photoelectric Equation: Energy Quantum of Radiation
- Particle Nature of Light: The Photon
- Wave Nature of Matter
Atoms
Nuclei
Semiconductor Electronics - Materials, Devices and Simple Circuits
Communication Systems
- Detection of Amplitude Modulated Wave
- Production of Amplitude Modulated Wave
- Basic Terminology Used in Electronic Communication Systems
- Sinusoidal Waves
- Modulation and Its Necessity
- Amplitude Modulation (AM)
- Need for Modulation and Demodulation
- Satellite Communication
- Propagation of EM Waves
- Bandwidth of Transmission Medium
- Bandwidth of Signals
The Special Theory of Relativity
- The Special Theory of Relativity
- The Principle of Relativity
- Maxwell'S Laws
- Kinematical Consequences
- Dynamics at Large Velocity
- Energy and Momentum
- The Ultimate Speed
- Twin Paradox
Iron Filings Reveal the Poles
When iron filings are sprinkled on a glass sheet placed over a bar magnet, they arrange themselves in curved lines running from one end of the magnet to the other. This pattern matches the electric field pattern around an electric dipole, which is why a bar magnet is called a magnetic dipole. The same pattern also appears around a current-carrying solenoid, hinting that magnets and electric currents produce the same type of field.
Types of Bar Magnets
| Type | Shape | Common Use |
|---|---|---|
| Cylindrical (rod) magnet | Thickness equal to or greater than diameter | Educational and research experiments |
| Rectangular magnet | Flat rectangular block | Manufacturing and engineering (stro |
Anatomy of a Bar Magnet
Picture a rectangular bar magnet lying horizontally:
- XX′ is the axis — an imaginary line running through both poles.
- YY′ is the equator — the perpendicular line through the magnet's centre.
- +qm is the pole strength of the North pole; −qm is the pole strength of the South pole (unit: A·m).
- D is the geometric length — the physical length you'd measure with a ruler.
- 2l is the magnetic length — the effective distance between the two poles used in calculations.
Key Fact: For every bar magnet, the magnetic length is about 84% of the geometric length: 2l / D = 0.84. Use this ratio unless a problem specifies otherwise.
Magnetic Dipole Moment
The magnetic dipole moment (m) measures how strongly a magnet can align with, or influence, a magnetic field. It always points from the South pole to the North pole, inside the magnet.
- SI Unit: Ampere-square metre (A·m2)
- Direction: South pole → North pole (inside the magnet)
Properties of a Bar Magnet
- Every bar magnet has two poles; breaking it never isolates a single pole — each piece becomes a smaller complete magnet.
- Magnetic force is strongest at the poles and weakest at the centre.
- A freely suspended magnet aligns its North pole toward Earth's magnetic north and its South pole toward Earth's magnetic south.
- Like poles repel; unlike poles attract.
- Bar magnets attract ferromagnetic materials (iron, steel, nickel, cobalt) that enter their field.
When You Cut a Bar Magnet
| Cutting Method | Pole Strength | Length | Result |
|---|---|---|---|
| Along the length (longitudinal) | Halved | Unchanged | Two thinner magnets, each with N and S poles |
| Across the length (transverse) | Unchanged | Halved | Two shorter magnets, each with N and S poles |
Common Misconception: Students often think cutting a magnet could produce an isolated N or S pole. In reality, magnetic monopoles do not exist — every fragment is a complete dipole.
Example
A bar magnet with pole strength qm, dipole length 2l, and magnetic moment m is cut along its length into two equal parts. Find the new pole strength and magnetic moment of each piece.
Solution: Cutting along the length halves the pole strength while the length stays the same.
Each half retains the original magnetic length but only half the pole strength, so its magnetic moment is exactly half the original.
Real Life Analogy
Think of a compass needle — it is simply a tiny bar magnet. When freely suspended, its North pole swings to point toward the Earth's geographic north, and its South pole points south, just like a full-size bar magnet would.
