Light polarization is a property of transverse waves that describes the orientation of the oscillations of the electric field vector in a specific direction perpendicular to the direction of wave propagation. Unpolarized light, such as sunlight, has electric field oscillations in all directions, while polarized light has oscillations confined to a single plane. Polarization is exploited in LCD screens, polarized sunglasses, photography filters, and scientific instruments like polarimeters.
I = I₀ × cos²(θ)
LaTeX: I = I_0 \cos^2\theta
| Symbol | Meaning | Unit |
|---|---|---|
| I | Transmitted intensity | W/m² |
| I₀ | Incident intensity after first polarizer | W/m² |
| θ | Angle between polarizer and analyzer | degrees or radians |
Problem
Unpolarized light of intensity I₀ = 80 W/m² passes through two polarizing filters. The first filter (polarizer) fully polarizes the light, and the second filter (analyzer) is oriented at 30° to the polarizer. What is the final intensity of light?
Solution
Step 1: After the first polarizer, intensity is halved (Malus's Law for unpolarized input). I₁ = I₀ / 2 = 80 / 2 = 40 W/m² Step 2: Apply Malus's Law for the second filter at θ = 30°. I₂ = I₁ × cos²(θ) I₂ = 40 × cos²(30°) I₂ = 40 × (√3/2)² = 40 × 0.75 = 30 W/m²
Answer
Final intensity = 30 W/m²
| Type | Method | Example | Plane of Oscillation |
|---|---|---|---|
| Linear Polarization | Polaroid filter or reflection | Polarized sunglasses | Single fixed plane |
| Circular Polarization | Quarter-wave plate | 3D cinema glasses | Rotates in a circle |
| Elliptical Polarization | Arbitrary wave plate | LCD displays | Rotates in an ellipse |
| Unpolarized Light | Natural emission | Sunlight, bulb light | All planes randomly |
| Partial Polarization | Partial reflection | Glare off water | Dominant + random planes |
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Light diffraction is the bending and spreading of light waves around obstacles or through narrow openings, occurring when the size of the aperture or obstacle is comparable to the wavelength of light. It is a consequence of the wave nature of light and produces characteristic interference patterns of alternating bright and dark fringes. Diffraction is fundamental to technologies such as diffraction gratings, X-ray crystallography, CD/DVD data storage, and optical microscopy resolution limits.
The refractive index (n) of a medium is a dimensionless number that describes how much slower light travels through that medium compared to its speed in a vacuum, defined as the ratio of the speed of light in vacuum to the speed of light in the medium. It also quantifies how much a ray of light bends (refracts) when entering the medium from vacuum, as described by Snell's Law. The refractive index determines critical phenomena such as total internal reflection, the sparkle of gemstones, and is essential in designing optical fibres, lenses, and camera systems.
The speed of light in vacuum, denoted by c, is a universal physical constant equal to exactly 299,792,458 metres per second, representing the maximum speed at which any information, energy, or matter can travel in the universe. As established by Albert Einstein's special theory of relativity (1905), c is invariant regardless of the motion of the source or observer. In transparent media such as glass or water, light travels at a reduced speed given by v = c/n, where n is the refractive index of the medium.
From Latin "polaris" (of the pole) and New Latin "polarizatio". The concept was formalized by French physicist Étienne-Louis Malus in 1808 when he discovered polarization by reflection.