Topics
Electric Charges and Fields
- Electric Charge
- Conductors and Insulators
- Basic 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
Electrostatics
Current Electricity
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
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
Electromagnetic Induction and Alternating Currents
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 Waves
Magnetism and Matter
Electromagnetic Induction
Optics
Dual Nature of Radiation and Matter
Alternating Current
Atoms and Nuclei
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 of Light Through a Prism
- Optical Instruments
- Microscope and it’s types
- Telescope
Wave Optics
- Concept of 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
Communication Systems
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
Introduction
When a force is conservative, work done against that force is stored as potential energy. In electrostatics, the Coulomb force between stationary charges is conservative, so a system of charges possesses electrostatic potential energy.
Definition: Electrostatic Potential Energy
Electrostatic potential energy is the energy stored in a system of charges due to their relative positions.
Core Idea: If an external force moves a test charge against the electrostatic force, the work done by the external agent is stored as electrostatic potential energy.
Charge Configuration
Consider a fixed point charge Q at the origin and a test charge q moved from point R to point P. If Q > 0 and q > 0, the electrostatic force is repulsive, so an external force must do work to bring the test charge closer.
Physical Meaning
- The electrostatic field opposes the inward motion of the positive test charge.
- The external force supplies energy to the system.
- That supplied energy appears as an increase in electrostatic potential energy.
Work Done and Potential Energy
If the test charge is moved from R to P, the work done by the external force is given by:
This work is stored as an increase in electrostatic potential energy.
Important Relation
The change in potential energy is: ΔU = UP − UR = WRP
This means the change in electrostatic potential energy equals the work done by the external force in moving the charge from R to P.
Meaning of the Result
Key Interpretation
- If external work is positive, electrostatic potential energy increases.
- If the electric field itself does the work, the system's potential energy decreases.
- Only the difference in potential energy between two points is physically significant.
Only the difference matters
An arbitrary constant may be added to potential energy without affecting physics, so the absolute value is not important; only the change in potential energy matters.
Zero of Potential Energy
The zero of electrostatic potential energy can be chosen conveniently. In electrostatics, it is commonly taken to be zero at infinity.
Standard Convention
If the potential energy at infinity is taken as zero, then the potential energy at a point is the work done in bringing the charge from infinity to that point.
Remember: In electrostatics, potential energy at infinity is usually taken as zero because the force becomes negligible at a very large distance.
Electrostatic Force is Conservative
A conservative force is one for which work done depends only on the initial and final positions, not on the path followed. The electrostatic force satisfies this condition.
Consequences
- Work done between two points is path-independent.
- A closed path has zero net work for electrostatic force.
- Electrostatic potential energy can be defined for a charge system.
Flowchart

Real-Life Understanding
Analogy 1: Pushing similar poles of magnets together
Bringing two like magnetic poles closer requires effort. In a similar way, bringing like charges closer requires external work, which gets stored as energy in the system.
Analogy 2: Lifting an object upward
Just as lifting a book increases its gravitational potential energy, bringing a positive charge closer to another positive charge increases electrostatic potential energy.
