How Does Thin Film Interference Affect Light Reflection?

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SUMMARY

The discussion focuses on the effects of thin film interference on light reflection, specifically involving a film with a thickness of 8.76 micrometers and a refractive index of 1.35. The incident light has a wavelength of 648 nm in air. The optical path length (OPL) is calculated as OPL = 2nt = 2(1.35)(8.76 x 103) nm, leading to the conclusion that approximately 36.5 wavelengths fit within the film's round trip. The phase difference between the two reflected waves is determined to be zero, resulting in constructive interference.

PREREQUISITES
  • Understanding of thin film interference principles
  • Familiarity with optical path length calculations
  • Knowledge of phase differences in wave reflections
  • Basic concepts of coherent light waves
NEXT STEPS
  • Study the derivation of the optical path length formula in thin films
  • Learn about the conditions for constructive and destructive interference
  • Explore the impact of varying refractive indices on light reflection
  • Investigate practical applications of thin film interference in optics
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Students in introductory physics courses, educators teaching optics, and anyone interested in understanding the principles of light behavior in thin films.

DottZakapa
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Homework Statement
Light with wave length 648 nm in air is incident perpendicularly from air on a film 8.76 micrometers think and with refractive index 1.35. par of the light is reflected from the first surface of the film, and part enters the film and is reflected back at the second surface where the fil is again in contact with air. How many waves are contained in its round trip through the film? What is the phase difference between these two parts of the light as they leave the film?
Relevant Equations
thin film
Homework Statement: Light with wave length 648 nm in air is incident perpendicularly from air on a film 8.76 micrometers think and with refractive index 1.35. par of the light is reflected from the first surface of the film, and part enters the film and is reflected back at the second surface where the fil is again in contact with air. How many waves are contained in its round trip through the film? What is the phase difference between these two parts of the light as they leave the film?
Homework Equations: thin film

the light incident on the film, having an index of refraction lower than the film has a phase difference of ##\frac{λ}{ 2}## the reflection from the second surface has no phase difference, therefore the formula for thin films in order to see a reflection would be

##2t=\frac{λ}{ 2}##

i don't understand how to answer the question... can anyone give some help?
 
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These problems are most easily done by introducing the optical path length which is ## OPL= 2nt =2(1.35)(8.76 \cdot 10^3 ) ## nm, rather than converting the wavelength in air to its wavelength in the material. Meanwhile ## \lambda =648 ## nm. The question should read "how many wavelengths..." and not how many waves. That calculation is of course quite simple, and is ## x=\frac{OPL}{\lambda} ##. ## \\ ## For the next part, the phase change from the reflection off the front surface is ## \pi ##, (which does correspond to half of a wavelength), but the correct way of saying the phase change is to call it ## \pi ## (radians).## \\ ## For the second question, they could be more descriptive, because the problem involves the interference of coherent light waves. Whatever result you get for ## x ##, you subtract off any integer, and just take any remaining fraction and multiply by ## 2 \pi ##. I did the arithmetic and this one turns out to be almost a round number. I'm going to bend the rules here, because I really can't explain the concepts properly without pretty much giving the answer at the same time. The arithmetic I did gave me ## x=36.5 ##. That is the answer to the first part of the problem, but when you answer the question about phase difference, the 36 gets dropped, (it accounts for a total phase of ## (36)(2 \pi) ##, but integers of ## 2 \pi ## have no effect on the interference). This leaves ## \phi_{back \, surface}= (.5)(2 \pi) =\pi ##, while ## \phi_{front \, surface}= \pi ##, so that there is a phase difference of ## \phi=0 ## between the two reflected waves, and thereby constructive interference. IMO, this problem is good for an example problem, but it is asking a lot of the students in an introductory class to solve it on their own.
 
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