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35.32. A plastic film with index of refraction 1.85 is put on the surface of a car window to increase the reflectivity and thus to keep the interior of the car cooler. The window glass has index of refraetion 1.52 . (a) What minimum thickness is required if light with wavelength 550 \(\mathrm{nm}\) in air reflected from the two sides of the film is to interfere constructively? (b) It is found to be difficult to manu- facture and install coatings as thin as calculated in part (a). What is the next greatest thickness for which there will also be constructive interference?

Short Answer

Expert verified
(a) 80.38 nm; (b) 160.76 nm.

Step by step solution

01

Understanding Constructive Interference Conditions

For two light waves to interfere constructively, the total phase difference between them must be an integer multiple of the wavelength. In the context of thin film interference, this condition for constructive interference when light reflects consecutively from the higher and then the lower refractive index is given by the equation: \( 2nt = m \lambda_n \), where \( n \) is the refractive index of the film, \( t \) is its thickness, \( m \) is the order of interference (an integer), and \( \lambda_n \) is the wavelength of light in the film. The wavelength of light in the film can be calculated by λ/n, where \( n \) is the refractive index.
02

Calculate Wavelength in Film

Given, the wavelength \( \lambda \) in air is 550 nm and the refractive index of the film \( n = 1.85 \). We calculate the wavelength of the light in the film: \( \lambda_n = \frac{550 \text{ nm}}{1.85} \approx 297.3 \text{ nm} \).
03

Finding Minimum Thickness for Constructive Interference (First Order)

To find the minimum thickness for constructive interference, use \( m = 1 \) in the equation \( 2nt = m \lambda_n \). Solve for \( t \):\[ 2(1.85)t = 1 \times 297.3 \]\[ t = \frac{297.3}{2 \times 1.85} \approx 80.38 \text{ nm} \].This is the minimum thickness required.
04

Find the Next Possible Thickness for Constructive Interference (Second Order)

To find the next greater thickness, consider the second order of interference, \( m = 2 \). Solve for \( t \) using the same formula:\[ 2(1.85)t = 2 \times 297.3 \]\[ t = \frac{2 \times 297.3}{2 \times 1.85} = \frac{594.6}{3.7} \approx 160.76 \text{ nm} \].

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Constructive Interference
When thinking about constructive interference in thin films, picture two waves meeting and reinforcing each other. This happens because their peaks and troughs align perfectly. In thin film interference, waves reflect off both the top and bottom surfaces of a film. For constructive interference, the path difference between these waves must be an integer multiple of the wavelength.

This condition is vital because it ensures that when the light reflects, it adds up instead of canceling out. The mathematical expression for constructive interference in thin films is:
  • \( 2nt = m \lambda_n \)
Here, \( n \) represents the refractive index of the film, \( t \) is the film's thickness, \( m \) is an integer (the order of interference), and \( \lambda_n \) is the wavelength of light within the film. Understanding this equation helps in calculating how thin or thick the film should be for colors to enhance rather than diminish.
Refractive Index
The refractive index is a measure of how much a material slows down light passing through it. Imagine light as a race car that suddenly encounters a slow zone; it'll move slower through the zone, which is similar to how light behaves passing through different substances.

When light enters a material like glass or plastic (our thin film), its speed and direction change. Different materials have different refractive indices, and this affects how light propagates in them. Our plastic film has a refractive index of 1.85, which means light travels slower in this plastic compared to air, which has a refractive index of about 1. The glass, part of the car window, has a refractive index of 1.52.
  • A higher refractive index means a higher "slowing down" of light.
  • This change in speed affects the wavelength of the light as it moves through the material.
Comprehending the refractive index is essential because it influences the wavelength within the medium, which is key to achieving the desired interference effects.
Wavelength in Medium
In air, light has a particular wavelength, but when it enters a medium like a thin plastic film, this wavelength shifts. This shift occurs because light travels slower in the medium due to its refractive index.

To find the new wavelength in the medium, we use the relationship:
  • \( \lambda_n = \frac{\lambda}{n} \)
Where \( \lambda \) is the original wavelength in air, and \( n \) is the refractive index of the medium. So, for our exercise, when light of 550 nm wavelength enters a plastic film of refractive index 1.85, the wavelength becomes approximately 297.3 nm.

Understanding this shift is critical because it determines how the light waves interact and create interference patterns. Calculating the wavelength within a medium helps in figuring out the thickness alterations necessary for achieving constructive interference.
Optical Coatings
Optical coatings, like those on car windows, are thin layers designed to change how light interacts with a surface. These coatings can enhance reflectivity, reduce reflection, or filter specific wavelengths.

This concept is particularly useful in managing energy efficiency and visibility. For instance, in the exercise, the plastic film coating on the car window enhances reflectivity, potentially cooling the car interior by reflecting more sunlight.

Key factors to consider about optical coatings include:
  • The refractive index of the coating material, which affects how much light is refracted.
  • The thickness of the coating, which determines what kind of interference (constructive or destructive) occurs for different wavelengths of light.
  • Manipulating the thickness can provide practical properties like anti-reflective or highly reflective surfaces.
Through the application of optical coatings, we can engineer surfaces that control light more effectively, creating products like glasses, camera lenses, and even cool automobile interiors.

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Most popular questions from this chapter

35.16. Coherent light of frequency \(6.32 \times 10^{14} \mathrm{Hz}\) passes through two thin slits and falls on a screen 85.0 \(\mathrm{cm}\) away. You observe that the third bright fringe occurs at \(\pm 3.11 \mathrm{cm}\) on either side of the central bright fringe. (a) How far apart are the two slits? (b) At what distance from the central bright fringe will the third dark fringe occur?

35.1. Two coherent sources \(A\) and \(B\) of radio waves are 5.00 \(\mathrm{m}\) apart. Each source emits waves with wavelength 6.00 \(\mathrm{m}\) . Consider points along the line between the two sources. At what distances, if any, from \(A\) is the interference (a) constructive and (b) destructive?

35.11. Coherent light from a sodium-vapor lamp is passed through a filter that blocks everything except light of a single wavelength. It then falls on two slits separated by 0.460 \(\mathrm{mm}\) . In the resulting interference pattern on a screen 2.20 \(\mathrm{m}\) away, adjacent bright fringes are separated by 2.82 \(\mathrm{mm}\) . What is the wavelength?

35.15. Coherent light with wavelength 600 \(\mathrm{nm}\) passes through two very narrow slits and the interference pattern is observed on a screen 3.00 \(\mathrm{m}\) from the slits. The first-order bright fringe is at 4.84 \(\mathrm{mm}\) from the center of the central bright fringe. For what wavelength of light will the first order dark fringe be observed at this same point on the screen?

35.28. Nonglare Glass. When viewing a piece of art that is behind glass, one often is affected by the light that is reflected off the front of the glass (called glare), which can make it difficult to see the art clearly. One solution is to coat the outer surface of the glass with a film to cancel part of the glare. (a) If the glass has a refractive index of 1.62 and you use \(\mathrm{TiO}_{2}\) , which has an index of refraction of \(2.62,\) as the coating, what is the minimum film thickness that will cancel light of wavelength 505 \(\mathrm{nm}\) ? (b) If this coating is too thin to stand up to wear, what other thickness would also work? Find only the three thinnest ones.

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