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
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
Electromagnetic Induction and Alternating Currents
Moving Charges and Magnetism
- Electromagnetism
- Magnetic force
- Motion in a Magnetic Field
- Magnetic Field Due to a Current Element, Biot-savart Law
- Magnetic Field on 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
Optics
Electromagnetic Induction
Alternating Current
Dual Nature of Radiation and Matter
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
- Overview of Ray Optics and Optical Instruments
Communication Systems
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
- Overview: Wave Optics
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
- Overview: Dual Nature of Radiation and Matter
The Special Theory of Relativity
Atoms
Nuclei
- Atomic Masses and Composition of Nucleus
- Size of the Nucleus
- Mass - Energy
- Nuclear Binding Energy
- Nuclear Force
- Radioactivity
- Forms of Energy > Nuclear Energy
- Nuclear Fission
- Nuclear Fusion
- Controlled Thermonuclear Fusion
- Overview: Nuclei
Semiconductor Electronics - Materials, Devices and Simple Circuits
- Concept of Semiconductor Electronics
- Classification of Metals, Conductors and Semiconductors
- Intrinsic Semiconductor
- Extrinsic Semiconductor
- n-type Semiconductor
- p-type Semiconductor
- Diode or p-n Junction
- Semiconductor Diode
- Application of Junction Diode as a Rectifier
- Overview: Semiconductor Electronics
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
A spherical refracting surface is a curved boundary separating two transparent media, where one medium has refractive index n1 and the other has refractive index n2.
When light travels from one medium to another through this curved surface, the rays bend due to refraction, and an image is formed depending on the curvature of the surface and the refractive indices of the two media.
This concept forms the basis for understanding lenses, because a thin lens may be treated as a combination of two spherical refracting surfaces.
Formula: Refraction at a Spherical Surface
For refraction at a spherical surface, the relation is:
\[\frac{n_2}{v}-\frac{n_1}{u}=\frac{n_2-n_1}{R}\]
Geometrical Setup
Consider an object point O placed on the principal axis of a spherical surface separating medium 1 and medium 2.
- Medium 1 has a refractive index n1.
- Medium 2 has a refractive index n2.
- The centre of curvature is C.
- The object distance is u.
- The image distance is v.
- The radius of curvature is R.

| Step | Action | Significance |
|---|---|---|
| 1 | A light ray travels from an object to a spherical boundary. | Establishes incident medium. |
| 2 | Ray strikes a curved surface and refracts. | Bending depends on refractive indices. |
| 3 | Refracted rays meet or appear to meet. | This determines the image position. |
| 4 | Formula links u, v, R, n₁, n₂. | Used for solving numericals. |
Cartesian Sign Convention
- All distances are measured from the pole.
- Distances measured in the direction of incident light are taken as positive.
- Distances measured opposite to the direction of incident light are taken as negative.
- Heights above the principal axis are positive.
- Heights below the principal axis are negative.
| Quantity | Sign rule | Typical case |
|---|---|---|
| u | Usually negative for a real object placed to the left of the surface. | Most board numericals |
| v | Positive for real image on the right, negative for virtual image on the left. | Depends on the image formed |
| R | Positive if the centre of curvature lies on the positive side, negative otherwise. | Depends on the surface shape |
Conceptual Understanding
When Light Goes from a Rarer to a Denser Medium
The refracted ray bends towards the normal, and the image position depends on the curvature of the spherical surface and the object location.
When Light Goes from a Denser to a Rarer Medium
The refracted ray bends away from the normal, and the image may shift differently for the same object distance because the refractive index contrast changes.
Real-Life Analogy
Looking through a curved glass bowl or a transparent marble gives a distorted view of an object because light is refracted at a curved surface rather than a flat one.
Derivation Outline
Stepwise Logic
- Consider a paraxial ray from object O incident on the spherical surface.
- Draw the normal at the point of incidence by joining that point to the centre of curvature C.
- Use the small-angle approximation for the angles made by the incident ray, refracted ray, and normal.
- Apply the refraction relation in its small-angle form.
- Rearrange terms in terms of u, v, and R.
- Obtain the standard formula for refraction at a spherical surface.
Plane Surface vs Spherical Surface Refraction
| Feature | Plane Surface | Spherical Surface |
|---|---|---|
| Boundary shape | Flat interface | Curved interface forming part of a sphere. |
| Image shift | The apparent depth type effect is common | Image location depends on curvature and refractive indices. |
| Main variables | Refractive indices and depth | u, v, R, n₁, n₂. |
Example
An object is placed at a distance of 100 cm in air from a convex spherical surface of glass of refractive index 1.5. The radius of curvature is 20 cm. Find the image distance.
Given
- n1 = 1 for air.
- n2 = 1.5 for glass.
- u = −100 cm.
- R = +20 cm.
Formula
Substitution
\[ \frac{1.5}{v} - \frac{1}{100} = \frac{0.5}{20} \]
\[ \frac{1.5}{v} + \frac{1}{100} = \frac{1}{40} \]
\[ \frac{1.5}{v} = \frac{1}{40} - \frac{1}{100} = \frac{3}{200} \]
\[ v = 100\ \text{cm} \]
Result
The image is formed 100 cm from the spherical surface inside the glass medium.
