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
Reflection of a Plane Wave by a Plane Surface
A plane wave AB is incident at an angle i on a reflecting surface MN. If v is the speed of the wave in the medium and τ is the time taken by the wavefront to advance from point B to C, then:
To construct the reflected wavefront, a sphere of radius vτ is drawn from point A. From point C, a tangent plane CE is drawn to this sphere. Then:
AB and CE represent the incident and reflected wavefronts, respectively. Considering triangles EAC and BAC, they are congruent, so the angles i and r are equal. Therefore, this gives the law of reflection.
Behaviour of Wavefronts
Once the laws of reflection and refraction are known, the behaviour of prisms, lenses, and mirrors can be understood. The source explains only the behaviour of wavefronts as they undergo reflection or refraction.
Plane Wave Through a Thin Prism
- A plane wave passes through a thin prism.
- The speed of light waves is less in glass.
- The lower portion of the incoming wavefront travels through the greatest thickness of glass and gets delayed more.
- This causes a tilt in the emerging wavefront.
Plane Wave Through a Thin Convex Lens
- A plane wave is incident on a thin convex lens.
- The central part of the incident plane wave passes through the thickest portion of the lens and is delayed the most.
- The emerging wavefront has a depression at the centre.
- Therefore, the wavefront becomes spherical and converges to point F, called the focus.
Plane Wave Reflected by a Concave Mirror
- A plane wave is incident on a concave mirror.
- On reflection, a spherical wave is formed.
- This spherical wave converges to the focal point F.
Similar Understanding
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Similarly, refraction and reflection by concave lenses and convex mirrors can be understood.
Equal Time Along Rays
From the discussion, the total time taken from a point on the object to the corresponding point on the image is the same when measured along any ray.
For example, when a convex lens focuses light to form a real image:
- The ray going through the centre travels a shorter path.
- But the speed is slower in glass.
- Therefore, the time taken is the same as for rays travelling near the edge of the lens.
Different rays may travel different paths, but the total time from object point to image point remains the same.
Example
Questions
a. When monochromatic light is incident on a surface separating two media, the reflected and refracted light both have the same frequency as the incident frequency. Explain why.
b. When light travels from a rarer to a denser medium, the speed decreases. Does the reduction in speed imply a reduction in the energy carried by the light wave?
c. In the wave picture of light, the intensity of light is determined by the square of the amplitude of the wave. What determines the intensity of light in the photon picture of light?
Solutions
a. Same Frequency of Reflected and Refracted Light
Reflection and refraction arise through the interaction of incident light with the atomic constituents of matter. Atoms may be viewed as oscillators that take up the frequency of an external agency, resulting in forced oscillations. The frequency of light emitted by a charged oscillator equals its frequency of oscillation. Thus, the frequency of scattered light equals that of the incident light.
b. Energy and Speed
No. Energy carried by a wave depends on the amplitude of the wave, not on the speed of wave propagation.
c. Intensity in the Photon Picture
For a given frequency, the intensity of light in the photon picture is determined by the number of photons crossing a unit area per unit time.

