Topics
Circular Motion
- Angular Displacement
- Angular Velocity
- Angular Acceleration
- Angular Velocity and Its Relation with Linear Velocity
- Uniform Circular Motion (UCM)
- Radial Acceleration
- Dynamics of Uniform Circular Motion - Centripetal Force
- Centrifugal Forces
- Banking of Roads
- Vertical Circular Motion Due to Earth’s Gravitation
- Equation for Velocity and Energy at Different Positions of Vertical Circular Motion
- Kinematical Equations for Circular Motion in Analogy with Linear Motion.
Rotational Dynamics
- Rotational Dynamics
- Circular Motion and Its Characteristics
- Applications of Uniform Circular Motion
- Vertical Circular Motion
- Moment of Inertia as an Analogous Quantity for Mass
- Radius of Gyration
- Theorems of Perpendicular and Parallel Axes
- Angular Momentum or Moment of Linear Momentum
- Expression for Torque in Terms of Moment of Inertia
- Conservation of Angular Momentum
- Rolling Motion
- Overview: Rotational Dynamics
Gravitation
- Newton’s Law of Gravitation
- Periodic Time
- Kepler’s Laws
- Binding Energy and Escape Velocity of a Satellite
- Weightlessness
- Variation of ‘G’ Due to Lattitude and Motion
- Variation in the Acceleration>Variation in Gravity with Altitude
- Communication satellite and its uses
- Composition of Two S.H.M.’S Having Same Period and Along Same Line
Mechanical Properties of Fluids
- Fluid and Its Properties
- Thrust and Pressure
- Pressure of liquid
- Pressure Exerted by a Liquid Column
- Atmospheric Pressure
- Gauge Pressure and Absolute Pressure
- Hydrostatic Paradox
- Pascal’s Law
- Application of Pascal’s Law
- Measurement of Atmospheric Pressure
- Mercury Barometer (Simple Barometer)
- Open Tube Manometer
- Surface Tension
- Molecular Theory of Surface Tension
- Surface Tension and Surface Energy
- Angle of Contact
- Effect of Impurity and Temperature on Surface Tension
- Excess Pressure Across the Free Surface of a Liquid
- Explanation of Formation of Drops and Bubbles
- Capillarity and Capillary Action
- Fluids in Motion
- Critical Velocity and Reynolds Number
- Viscous Force or Viscosity
- Stokes’ Law
- Terminal Velocity
- Continuous and Discontinuous Functions
- Bernoulli's Equation
- Applications of Bernoulli’s Equation
- Overview: Mechanical Properties of Fluids
Kinetic Theory of Gases and Radiation
- Gases and Its Characteristics
- Classification of Gases: Real Gases and Ideal Gases
- Mean Free Path
- Expression for Pressure Exerted by a Gas
- Root Mean Square (RMS) Speed
- Interpretation of Temperature in Kinetic Theory
- Law of Equipartition of Energy
- Specific Heat Capacity
- Absorption, Reflection, and Transmission of Heat Radiation
- Perfect Blackbody
- Emission of Heat Radiation
- Kirchhoff’s Law of Heat Radiation and Its Theoretical Proof
- Spectral Distribution of Blackbody Radiation
- Wien's Displacement Law
- Stefan-boltzmann Law of Radiation
- Overview: Kinetic Theory of Gases and Radiation
Angular Momentum
- Definition of M.I., K.E. of Rotating Body
- Rolling Motion
- Physical Significance of M.I (Moment of Inertia)
- Torque and Angular Momentum
- Theorems of Perpendicular and Parallel Axes
- M.I. of Some Regular Shaped Bodies About Specific Axes
Oscillations
- Periodic and Oscillatory Motion
- Simple Harmonic Motion (S.H.M.)
- Differential Equation of Linear S.H.M.
- Projection of U.C.M.(Uniform Circular Motion) on Any Diameter
- Phase of K.E (Kinetic Energy)
- K.E.(Kinetic Energy) and P.E.(Potential Energy) in S.H.M.
- Composition of Two S.H.M.’S Having Same Period and Along Same Line
- Some Systems Executing Simple Harmonic Motion
Thermodynamics
- Thermodynamics
- Thermal Equilibrium
- Measurement of Temperature
- Heat, Internal Energy and Work
- First Law of Thermodynamics
- Thermodynamic State Variables and Equation of State
- Thermodynamic Process
- Heat Engine
- Refrigerators and Heat Pumps
- Entropy and Second Law of Thermodynamics
- Carnot Cycle and Carnot Engine
- Overview: Thermodynamics
Elasticity
- Eneral Explanation of Elastic Property
- Stress and Strain
- Hooke’s Law
- Elastic Energy
- Elastic Constants and Their Relation
- Determination of ‘Y’
- Behaviour of Metal Wire Under Increasing Load
- Application of Elastic Behaviour of Materials
Oscillations
- Oscillations
- Explanation of Periodic Motion
- Linear Simple Harmonic Motion (S.H.M.)
- Differential Equation of Linear S.H.M.
- Acceleration (a), Velocity (v) and Displacement (x) of S.H.M.
- Amplitude (A), Period (T) and Frequency (N) of S.H.M.
- Reference Circle Method
- Phase in S.H.M.
- Graphical Representation of S.H.M.
- Composition of Two S.H.M.’S Having Same Period and Along Same Line
- The Energy of a Particle Performing S.H.M.
- Simple Pendulum
- Angular S.H.M. and It's Differential Equation
- Damped Oscillations
- Free Oscillations, Forced Oscillations and Resonance Oscillations
- Periodic and Oscillatory Motion
- Overview: Oscillations
Surface Tension
- Molecular Theory of Surface Tension
- Surface Tension
- Capillarity and Capillary Action
- Effect of Impurity and Temperature on Surface Tension
Superposition of Waves
Wave Motion
- Wave Motion Introduction
- Simple Harmonic Progressive Waves,
- Reflection of Transverse and Longitudinal Waves
- Change of Phase
- Principle of Superposition of Waves
- Formation of Beats
- Beats
Wave Optics
- Concept of Wave Optics
- Nature of Light
- Light as a Wave
- Huygens Principle
- Reflection of Light at a Plane Surface
- Refraction of Light at a Plane Boundary Between Two Media
- Polarisation of Light
- Interference
- Diffraction of Light
- Resolving Power
- Overview: Wave Optics
Stationary Waves
- Study of Vibrations in a Finite Medium
- Formation of Stationary Waves on String
- Study of Vibrations of Air Columns
- Free and Forced Vibrations
- Forced Oscillations and Resonance
Electrostatics
- Concept of Electrostatics
- Application of Gauss' Law
- Electric Potential and Potential Difference
- Electric Potential Due to a Point Charge
- Equipotential Surfaces
- Electrical Energy of Two Point Charges and of a Dipole in an Electrostatic Field
- Free Charges and Bound Charges Inside a Conductor
- Combination of Capacitors
- Displacement Current
- Energy Stored in a Charged Capacitor
- Van De Graaff Generator
- Uniformly Charged Infinite Plane Sheet and Uniformly Charged Thin Spherical Shell (Field Inside and Outside)
- Overview: Electrostatics
Kinetic Theory of Gases and Radiation
- Concept of an Ideal Gas
- Assumptions of Kinetic Theory of Gases
- Derivation for Pressure of a Gas
- Degrees of Freedom
- Derivation of Boyle’s Law
- Thermal Equilibrium
- First Law of Thermodynamics
- Heat Engine
- Temperature and Heat
- Qualitative Ideas of Black Body Radiation
- Wien's Displacement Law
- Green House Effect
- Stefan's Law
- Maxwell Distribution
- Specific Heat Capacities - Gases
- Law of Equipartition of Energy
Current Electricity
Wave Theory of Light
Magnetic Fields Due to Electric Current
- Magnetic Fields Due to Electric Current
- Magnetic force
- Cyclotron
- Helical Motion
- Magnetic Force on a Wire Carrying a Current
- Force on a Closed Circuit in a Magnetic Field
- Torque on a Current-Loop in a Uniform Magnetic Field
- Magnetic Dipole Moment
- Magnetic Potential Energy of a Dipole
- Magnetic Field Due to a Current Element, Biot-savart Law
- Force of Attraction Between Two Long Parallel Wires
- Magnetic Field Produced by a Current in a Circular Arc of a Wire
- Magnetic Field on the Axis of a Circular Current-Carrying Loop
- Magnetic Lines for a Current Loop
- Ampere’s Circuital Law
- Applications of Ampere’s Circuital Law > Magnetic Field of a Toroidal Solenoid
- Overview: Magnetic Fields Due to Electric Current
Interference and Diffraction
- Interference of Light
- Conditions for Producing Steady Interference Pattern
- Interference of Light Waves and Young’s Experiment
- Analytical Treatment of Interference Bands
- Measurement of Wavelength by Biprism Experiment
- Fraunhofer Diffraction Due to a Single Slit
- Rayleigh’s Criterion
- Resolving Power of a Microscope and Telescope
- Difference Between Interference and Diffraction
Magnetic Materials
- Magnetic Materials
- Torque Acting on a Magnetic Dipole in a Uniform Magnetic Field
- Origin of Magnetism in Materials
- Magnetisation and Magnetic Intensity
- Magnetic Properties of Materials
- Classification of Magnetic Materials
- Hysteresis: Retentivity and Coercivity
- Permanent Magnet
- Magnetic Shielding
- Overview: Magnetic Materials
Electromagnetic Induction
- Electromagnetic Induction
- Faraday's Laws of Electromagnetic Induction
- Lenz's Law
- Flux of a Vector Field
- Motional Electromotive Force (e.m.f.)
- Induced Emf in a Stationary Coil in a Changing Magnetic Field
- Generators
- Back Emf and Back Torque
- Induction and Energy Transfer
- Eddy Currents or Foucault Currents
- Self Inductance
- Energy Stored in a Magnetic Field
- Energy Density of a Magnetic Field
- Mutual Inductance
- Transformers
- Overview of Electromagnetic Induction
Electrostatics
- Mechanical Force on Unit Area of a Charged Conductor
- Energy Density of a Medium
- Concept of Condenser
- The Parallel Plate Capacitor
- Capacity of Parallel Plate Condenser
- Effect of Dielectric on Capacitance
- Energy of Charged Condenser
- Condensers in Series and Parallel,
- Van-deGraaff Generator
AC Circuits
- AC Circuits
- Values of Alternating Current
- Phasors
- AC Voltage Applied to a Resistor
- AC Voltage Applied to an Inductor
- AC Voltage Applied to a Capacitor
- AC Voltage Applied to a Series LCR Circuit
- Power in AC Circuit
- LC Oscillations
- Electric Resonance
- Sharpness of Resonance: Q Factor
- Choke Coil
- Overview: AC Circuits
Current Electricity
- Meter Bridge
Dual Nature of Radiation and Matter
Magnetic Effects of Electric Current
Magnetism
Structure of Atoms and Nuclei
- Structure of the Atom and Nucleus
- Thomson’s Atomic Model
- Geiger-marsden Experiment
- Lord Rutherford’s Atomic model
- Atomic Spectra
- Neils Bohr’s Model of an Atom
- Atomic Nucleus
- Constituents of a Nucleus
- Isotopes
- Atomic and Nuclear Masses
- Size of the Nucleus
- Mass Defect and Binding Energy
- Binding Energy Curve
- Forms of Energy > Nuclear Energy
- Nuclear Binding Energy
- Radioactive Decays
- Law of Radioactive Decay
- Overview: Structure of Atoms and Nuclei
Electromagnetic Inductions
- Electromagnetic Induction
- Self Inductance
- Mutual Inductance
- Transformers
- Need for Displacement Current
- Coil Rotating in Uniform Magnetic Induction
- A.C. Generator
- Reactance and Impedance
- LC Oscillations
- Inductance and Capacitance
- Resonant Circuits
- Power in AC Circuit
- Lenz’s Law and Conservation of Energy
Semiconductor Devices
Electrons and Photons
Atoms, Molecules and Nuclei
- Alpha-particle Scattering and Rutherford’s Nuclear Model of Atom
- Bohr’s Model for Hydrogen Atom
- Hydrogen Spectrum
- Atomic Masses and Composition of Nucleus
- Radioactivity
- Law of Radioactive Decay
- Atomic Mass, Mass - Energy Relation and Mass Defect
- Nuclear Binding Energy
- Nuclear Fusion
- de-Broglie Relation
- Wave Nature of Matter
- Wavelength of an Electron
- Davisson and Germer Experiment
- Continuous and Characteristics X-rays
- Mass Defect and Binding Energy
Semiconductors
- Energy Bands in Solids
- Extrinsic Semiconductor
- Applications of n-type and p-type Semiconductors
- Special Purpose P-n Junction Diodes
- Semiconductor Diode
- Voltage Regulator
- I-V Characteristics of Led
- Transistor and Characteristics of a Transistor
- Transistor as an Amplifier (Ce-configuration)
- Transistor as a Switch
- Oscillators
- Digital Electronics and Logic Gates
Communication Systems
Introduction
Faraday's laws of electromagnetic induction establish that whenever the magnetic flux through a closed circuit changes, an EMF is induced in the circuit. Faraday's laws determine the magnitude of this induced EMF.
Lenz's Law was formulated by German physicist Heinrich Friedrich Emil Lenz in 1834. Lenz's law is not an independent principle — it is a direct physical consequence of the Law of Conservation of Energy. Together, Faraday's laws and Lenz's law form the complete framework of electromagnetic induction.
Definition: Lenz's Law
The direction of the induced EMF (and hence the induced current) in a closed conducting loop is always such that it opposes the change in magnetic flux that produced it.
Formula: Lenz's Law
The mathematical form of Faraday's law with Lenz's law incorporated is
\[\varepsilon=-N\frac{d\Phi_B}{dt}\]
Experiment:
Apparatus: Bar magnet, coil of wire, and galvanometer connected to the coil.
Observations:
| Action | Flux Change | Galvanometer | Induced Current Direction | Face of Coil (near magnet) |
|---|---|---|---|---|
| The N-pole moved towards the coil | Increases ↑ | Deflects | Anticlockwise (viewed from the magnet) | North pole — repels magnet |
| Magnet held stationary | No change | No deflection | No current | — |
| The N-pole moved away from the coil | Decreases ↓ | Deflects (opposite direction) | Clockwise (viewed from the magnet) | South pole — attracts a magnet |
| The S-pole moved towards the coil | Increases ↑ | Deflects | Clockwise (viewed from the magnet) | South pole — repels magnet |
| The S-pole moved away from the coil | Decreases ↓ | Deflects (opposite direction) | Anticlockwise (viewed from the magnet) | The North Pole attracts a magnet |
Conclusion from experiment: In every case, the induced current creates a magnetic pole on the face of the coil that opposes the motion of the magnet — confirming Lenz's law. Work must always be done by an external agent to move the magnet, and this work is the source of the electrical energy.
Law: Lenz's Law
Statement
The induced EMF in a closed loop has a direction such that the current it drives would create a magnetic flux to oppose the change in flux through the circuit.
Mathematically, this is captured by the negative sign:
Proof (Lenz's Law as Conservation of Energy)
Claim: Lenz's law is a necessary consequence of the Law of Conservation of Energy.
Proof by contradiction:
Suppose, contrary to Lenz's law, the induced current aided the change in flux instead of opposing it.
- When the N-pole of a magnet approaches a coil, the induced current (if aiding) would create a South pole on the near face of the coil
- This South pole would attract the incoming North pole of the magnet
- The magnet would accelerate towards the coil without any external effort
- The accelerating magnet would induce more current, which would attract the magnet even more strongly
- This would result in continuously increasing kinetic energy and electrical energy, generated from nothing
- This is a perpetual motion machine — a direct violation of the Law of Conservation of Energy
Since this is impossible, the induced current must oppose the flux change — Lenz's law is proved.
Conclusion
- Lenz's law is not an arbitrary rule — it is mandated by energy conservation
- The work done by the external agent (to overcome the opposing electromagnetic force) is the source of all electrical energy generated
- Without Lenz's law, electromagnetic induction would violate the most fundamental law of physics
Understanding the Opposition
This is the most misunderstood aspect of Lenz's law.
Lenz's law does not oppose the existing magnetic flux. A coil sitting inside a strong, steady magnetic field has no induced current
Lenz's law opposes the change in flux — meaning it opposes:
- An increase in flux (by generating an opposing field)
- A decrease in flux (by generating a supporting field to maintain it)
The Direction Rule
To find the direction of the induced current in any situation:
1. Identify the direction of the original magnetic field B through the loop
2. Determine whether ΦB is increasing or decreasing
3. Apply Lenz's law:
- If ΦB is increasing, → induced B must point opposite to the original B inside the loop
- If ΦB decreases, induced B must point in the same direction as the original B inside the loop
4. Use Right-Hand Thumb Rule: Curl fingers of right hand in the direction of induced current → thumb points in direction of induced B
Lenz's Law as Electromagnetic Inertia
Lenz's law behaves like electromagnetic inertia — just as Newton's first law says a body resists changes in its state of motion, Lenz's law says an electromagnetic circuit resists changes in its magnetic flux. The greater the rate of change of flux, the stronger the induced current and the stronger the opposing force.
Real-Life Applications
| Application | Principle (Lenz’s Law in Action) |
|---|---|
| Electromagnetic Brakes(high-speed trains, roller coasters) | Eddy currents induced in metal discs by a changing magnetic field oppose the disc's motion, resulting in contactless, wear-free braking. |
| AC Generators | As the coil rotates, the induced EMF opposes the rotation (back EMF). Continuous mechanical work must be supplied to maintain rotation. |
Example
The Question: Three loops of different shapes (rectangular, triangular, irregular) are either moving into or out of a magnetic field region. The field points away from you (out of the page). Find the direction of the induced current in each loop using Lenz's law.
Loop (i) — Rectangular Loop Moving INTO the Field
| Step | What Happens |
|---|---|
| Step 1: What is the loop doing? | Moving into the magnetic field region. |
| Step 2: What happens to the flux? | Magnetic flux through the loop increases because more magnetic field lines pass through the loop. |
| Step 3: Apply Lenz’s Law | The induced current must oppose the increase in flux. Therefore, it must produce a magnetic field directed into the page, opposite to the existing field, which is out of the page. |
| Step 4: Use the Right-Hand Rule | To produce an induced magnetic field inside the loop, the induced current must flow clockwise. |
| Answer | Current flows along the path b → c → d → a → b. |
Loop (ii) — Triangular Loop Moving OUT of the Field
| Step | What Happens |
|---|---|
| Step 1: What is the loop doing? | Moving out of the magnetic field region. |
| Step 2: What happens to the flux? | Magnetic flux through the loop decreases because fewer magnetic field lines pass through the loop. |
| Step 3: Apply Lenz’s Law | The induced current must oppose the decrease in flux. Therefore, it must produce a magnetic field directed out of the page, in the same direction as the existing magnetic field, to maintain the flux. |
| Step 4: Use the Right-Hand Rule | To produce an induced magnetic field out of the page inside the loop, the induced current must flow anticlockwise. |
| Answer | Current flows along the path b → a → c → b. |
Loop (iii) — Irregular Loop Moving OUT of the Field
| Step | What Happens |
|---|---|
| Step 1: What is the loop doing? | Moving out of the magnetic field region. |
| Step 2: What happens to the flux? | Magnetic flux through the loop decreases. |
| Step 3: Apply Lenz’s Law | The induced current opposes the decrease in flux by producing a magnetic field directed out of the page. |
| Step 4: Answer | Current flows along the path c → d → a → b → c. |






