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Question: White light is incident normally on a glass plate of thickness 0.50 × $10^{-6}$ and index of refract...

White light is incident normally on a glass plate of thickness 0.50 × 10610^{-6} and index of refraction 1.50. Which wavelengths in the visible region (400 nm-700 nm) are strongly reflected by the plate?

Answer

500 nm

Explanation

Solution

The phenomenon is thin-film interference. For normal incidence, the optical path difference (OPD) between the two reflected rays is 2μt2\mu t.

Given: Thickness of the plate, t=0.50×106t = 0.50 \times 10^{-6} m Refractive index of the plate, μ=1.50\mu = 1.50 Visible light range: λ[400nm,700nm]\lambda \in [400 \, \text{nm}, 700 \, \text{nm}].

The optical path difference is: 2μt=2×1.50×(0.50×106m)=1.5×106m=1500nm2\mu t = 2 \times 1.50 \times (0.50 \times 10^{-6} \, \text{m}) = 1.5 \times 10^{-6} \, \text{m} = 1500 \, \text{nm}.

Phase Shifts:

  1. Reflection at the first surface (air to glass): μglass>μair\mu_{glass} > \mu_{air}, so there is a phase change of π\pi.
  2. Reflection at the second surface (glass to air): μglass>μair\mu_{glass} > \mu_{air}, so there is a phase change of π\pi.

When both reflections involve a phase shift of π\pi, the condition for constructive interference (strong reflection) is 2μt=nλ2\mu t = n\lambda, where nn is an integer.

We need to find integer values of nn for which λ\lambda falls within the visible region (400 nm to 700 nm): λ=2μtn=1500nmn\lambda = \frac{2\mu t}{n} = \frac{1500 \, \text{nm}}{n}.

4001500n700400 \le \frac{1500}{n} \le 700

From 4001500n400 \le \frac{1500}{n}: n1500400=3.75n \le \frac{1500}{400} = 3.75. From 1500n700\frac{1500}{n} \le 700: n15007002.14n \ge \frac{1500}{700} \approx 2.14.

The possible integer value for nn is 33. For n=3n=3, λ=15003=500nm\lambda = \frac{1500}{3} = 500 \, \text{nm}.

Therefore, the wavelength strongly reflected is 500 nm.