#polarization

What causes the intensity to vary when a second polaroid is rotated in front of another polaroid through which unpolariz

**Convex lens focusing** plane wave into point because lens introduces phase delay proportional to thickness, converting plane wavefront to spherical converging to focal point, property ensures rays parallel to axis meet at focus, spherical aberration minimized for paraxial rays, lensmaker's formula determines focal length. The first polaroid polarizes the light linearly, and the second allows only the component of the electric field aligned with its pass-axis, varying with the angle via Malus’ law. Using Δ = d sinθ, y = n λ D/d, a sinθ = n λ, I = I₀ cos²θ, n = c/v, sinC = 1/n, λ' = λ/n and A

Ref: NCERT > Physics Book > Wave Optics > Optical Phenomena and Applications

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Optical Phenomena and Applications

What causes the intensity of light to vary sinusoidally with angle when passing through two polaroids?

**Polarization requires transverse waves** because only transverse can have orientation perpendicular to propagation, longitudinal cannot be polarized, wave theory requires light transverse to explain polarization, polaroids transmit only component along pass-axis, unpolarized has random transverse orientations, after polaroid polarized. The intensity follows Malus’ law, where it varies as the square of the cosine of the angle between the polaroids’ axes, producing a sinusoidal pattern. Using Δ = d sinθ, y = n λ D/d, a sinθ = n λ, I = I₀ cos²θ, n = c/v, sinC = 1/n, λ' = λ/n and A = 2a cos(φ/2)

Ref: NCERT > Physics Book > Wave Optics > Optical Phenomena and Applications

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Optical Phenomena and Applications

What is the intensity of light after passing through two polaroids with pass-axes at \( 45^\circ \), if the initial unpo

**Incoherent sources** intensity adds I = I₁+I₂, no interference pattern because phase random, two independent sources cannot produce stable interference because phase difference fluctuates rapidly, coherent sources required with constant phase, laser coherent, visibility of fringes requires coherence, degree of coherence determines contrast. After the first polaroid, I = (I₀/2) . After the second at 45° , I = (I₀/2) cos² 45° = (I₀/2) × (1/2) = (I₀/4) . Using Δ = d sinθ, y = n λ D/d, a sinθ = n λ, I = I₀ cos²θ, n = c/v, sinC = 1/n, λ' = λ/n and A = 2a cos(φ/2), calculation gives (I₀/4),

Ref: NCERT > Physics Book > Wave Optics > Optical Phenomena and Applications

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Polarization and Malus Law

Why does the intensity of light transmitted through two polaroids become zero when their axes are at 90° to each other?

**Polarization** transverse wave property, light after polaroid polarized along pass-axis, Malus law I = I₀ cos²θ, θ angle between pass-axes, initial unpolarized intensity I₀ after first polaroid I₁ = I₀/2, after second at 45° I₂ = I₁ cos²45°= I₀/2×0.5= I₀/4, after two perpendicular 90° I=0 because cos90°=0, for 60° I= I₀/2×cos²60°= I₀/2×0.25= I₀/8. The first polaroid aligns the electric field, and the second, perpendicular to it, blocks all components, as the cosine of 90° is zero in the intensity relation. Using Δ = d sinθ, y = n λ D/d, a sinθ = n λ, I = I₀ cos²θ, n = c/v, sinC = 1/n,