Topics
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
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
Magnetism and Matter
Electromagnetic Waves
Electromagnetic Induction
Optics
Dual Nature of Radiation and Matter
Alternating Current
Electromagnetic Waves
- Introduction to Electromagnetic Waves
- Displacement Current
- Sources of Electromagnetic Waves
- Nature of Electromagnetic Waves
- Electromagnetic Spectrum
- Definition and Characteristics of Electromagnetic Waves
Atoms and Nuclei
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
Electronic Devices
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
Communication Systems
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
The Special Theory of Relativity
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
Definition: Elementary Charge
The smallest unit of electric charge, denoted by e, is called the elementary charge.
Maharashtra State Board: Class 11
Point Charge
- Electric charges are considered very small, called point charges, to better understand their properties.
- If the sizes of charged bodies are very small compared to the distances between them, all the charge is assumed to be concentrated at one point in space.
Maharashtra State Board: Class 11
Additivity of Electric Charges
- Electric charges are scalar quantities — they have magnitude and sign but no direction.
- If a system has n charges, the total charge is the algebraic sum of all individual charges: Q = q1 + q2 + q3 + ... + qn
- Charges add up like real numbers — positive and negative signs must always be included while adding.
- Unlike mass (which is always positive), charge can be positive or negative.
- For example, five charges +1, +2, −3, +4, −5 give a total of: (+1) + (+2) + (−3) + (+4) + (−5) = −1 unit.
CISCE: Class 12
Key Points: Important Properties of Electric Charge
- Quantisation of charge: Electric charge exists in discrete packets, and the charge on any body is given by
q = ±ne
where n is an integer and e = 1.6 × 10−19 C is the elementary charge. - No fractional charge: Charge cannot exist as a fraction of eee (like 0.5e or 2.3e); hence, electric charge is atomic in nature.
- Conservation of charge: The total electric charge of an isolated system remains constant; charge can neither be created nor destroyed, only transferred.
- Experimental support: Processes such as rubbing, pair production and annihilation, and radioactive decay always conserve the net charge of the system.
- Invariance of charge: The value of electric charge does not change with velocity, unlike mass, which varies with speed.
Maharashtra State Board: Class 11
Conservation of Electric Charges
- Charges are neither created nor destroyed — they can only be transferred from one body to another.
- When two bodies are rubbed together, what one body gains in charge, the other body loses — no new charge is produced.
- In an isolated system, even if charges get redistributed among many bodies, the total charge always remains the same.
- Nature can create charged particles — for example, a neutron turns into a proton and an electron. The proton carries +e and the electron carries −e, so the total charge remains zero, just as it was before.
Definition: Point Charge
A charged body whose size is negligibly small compared to the distance between the charges under consideration, is called a point charge.
Maharashtra State Board: Class 11
Quantisation of Electric Charge
- All free charges are always an integer multiple of a basic unit of charge e: q = ne
where n is any integer (positive or negative). - The charge on an electron is −e and on a proton is +e.
- The value of the elementary charge is e = 1.602192 × 10−19 C.
- Quantisation of charge was first suggested by Faraday through electrolysis laws and experimentally demonstrated by Millikan in 1912.
- If a body has n1 electrons and n2 protons, its total charge is (n2 − n1) ⋅ e, always an integer multiple of e.
- At the macroscopic level, the step size e is so tiny that the charge appears continuous, like how a dotted line looks solid from a distance.
- At the microscopic level, charges are only a few multiples of e, so the discrete nature of charge cannot be ignored.
Example 1
Question: If 10⁹ electrons move out of a body every second, how long does it take to collect a total charge of 1 C?
Think of it this way: Imagine you are filling a large water tank, but your tap releases only a tiny drop every second. It will take a very, very long time to fill the tank. Similarly, each electron carries an incredibly tiny charge, so even 10⁹ (one billion) electrons leaving every second adds up to very little charge per second.
-
Charge leaving per second
= 109 × 1.6 × 10−19 C
= 1.6 × 10−10 C/s -
Time to collect 1 C = \[\frac {1}{1.6×10^{−10}}\] = 6.25 × 109 seconds = approximately 198 years
Conclusion: 1 Coulomb is an enormous amount of charge. Even with a billion electrons leaving every second, it would take about 200 years to gather just 1 C — this is why we use smaller units like μC in electrostatics.
Example 2
Question: How many positive and negative charges are there in a cup of water (250 g)?
Think of it this way: Every water molecule (H₂O) contains 2 hydrogen atoms and 1 oxygen atom — that gives 10 protons and 10 electrons per molecule. Both charges are equal and opposite, so they cancel out, and water is neutral. But if you count all those charges separately, the numbers are surprisingly huge.
-
Number of water molecules in 250 g = \[\frac {250}{18}\] × 6.02 × 1023
-
Each molecule has 10 protons (+) and 10 electrons (−)
-
Total positive charge = Total negative charge = \[\frac {250}{18}\] × 6.02 × 1023 × 10 × 1.6 × 10−19 ≈ 1.34 × 10⁷ C
Conclusion: A single cup of water contains about 13 million Coulombs of both positive and negative charge — they perfectly cancel each other, leaving the water electrically neutral. This shows that enormous charges exist in ordinary matter, completely balanced.
