Thin Film Interference Problem

In summary: One ray reflects from the front surface of the air gap with no phase change. The other ray traverses the air gap (1.5 λ), changing the phase by 3 pi, reflects from a denser medium, that changes the phase by pi, then traverses the gap again, so the net phase difference between the waves is 7pi. Odd number of pi, so the waves interfere destructively. In summary, using the first argument, the path difference between the waves is 3λ, which does not change the outcome of the interference. However, using the argument referring to the phase difference, the phase difference between the waves is 7pi, which means the waves will interfere constructively.
  • #1
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Homework Statement



Light strikes two plane sheets of glass with a thin air space between them as shown. If the light has a wavelength of 580 nm and the air space between the glass has a thickness of 870 nm, predict whether the reflected light as demonstrated by rays A and B will cancel or produce a bright spot.

Homework Equations



2t=mλ, m=1,2,3...


The Attempt at a Solution



So using the above equation, and substituting the values in the question, I obtain, m=3. So the path difference is 3λ (extra distance ray B travels)
Then since the second ray (ray B) is reflected from a denser medium (glass), it is in phase reversal or λ/2 out of phase. So, then the total path difference is 3.5 λ. Since its a half-integral multiple it implies the rays will cancel-produce a dark spot.
Is this logic correct?

I've been told this is the correct answer, but initially I would have said that the path difference is 3λ, since the rays are already out of phase-and destructive interference would occur-producing a dark spot. Then the whole integral number of wavelengths (3λ in this case), wouldn't change the status of the system, so the rays will cancel. But this is supposedly wrong, with the first answer being correct.
Can someone please clarify why this is true.
 
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  • #2
Both arguments are correct, integer number of wavelengths in the path difference do not count.

ehild
 
  • #3
ehild said:
Both arguments are correct, integer number of wavelengths in the path difference do not count.

ehild

Would you advise its better to use the first argument, or does it really not matter?
 
  • #4
I think the firs argument is better to use. But I prefer argument referring to phase difference. If the phase diference between two waves is odd number of pi, the interference is destructive, if it is even number of pi, it is constructive.

Travelling across λ distance changes the phase by 2pi. Reflecting from a denser medium changes the phase by pi.
One ray reflects from the front surface of the air gap with no phase change. The other ray traverses the air gap (1.5 λ), changing the phase by 3 pi, reflects from a denser medium, that changes the phase by pi, then traverses the gap again, so the net phase difference between the waves is 7pi. Odd number of pi, so the waves interfere destructively.


ehild
 
  • #5


I would like to clarify that both of your answers are correct. The first answer, where you calculated the path difference to be 3.5λ, is based on the assumption that the light is incident normally on the glass sheets. In this case, the rays A and B will indeed cancel each other out and produce a dark spot.

However, the second answer is also valid if we consider the possibility that the light may not be incident normally on the glass sheets. In this case, the path difference would be exactly 3λ and the rays would still cancel out and produce a dark spot. So, in essence, both answers are correct and it depends on the specific conditions of the experiment.

Additionally, it is important to note that thin film interference is a complex phenomenon and can be affected by various factors such as the angle of incidence, the refractive index of the materials, and the polarization of the light. Therefore, it is important to consider all these factors when predicting the outcome of an interference problem.

In conclusion, your logic and understanding of thin film interference is correct, and it is important to consider all the relevant factors when solving such problems. I hope this clarifies any confusion and helps you to further your understanding of this concept.
 

What is thin film interference?

Thin film interference is a phenomenon that occurs when light waves reflect off of the upper and lower surfaces of a thin film at different angles, causing them to interfere with each other. This results in a change in the overall intensity and color of the light that is transmitted or reflected by the film.

What causes thin film interference?

Thin film interference is caused by the difference in the path length that light waves travel when reflecting off of the upper and lower surfaces of a thin film. This difference in path length leads to constructive or destructive interference, depending on the thickness of the film and the wavelength of the light.

What is the difference between thin film interference and thick film interference?

The main difference between thin film interference and thick film interference is the thickness of the film itself. Thin film interference occurs when the film is much thinner than the wavelength of the light, while thick film interference occurs when the film is thicker than the wavelength of the light.

How is thin film interference used in practical applications?

Thin film interference has many practical applications in various industries, such as in the production of anti-reflective coatings for eyeglasses and camera lenses, in the creation of colorful optical filters, and in the development of advanced optical devices such as interferometers and spectrometers.

How can thin film interference be controlled or manipulated?

Thin film interference can be controlled or manipulated by changing the thickness of the film, the angle of incidence of the light, or the refractive index of the film material. These changes can alter the path length difference and thus the interference pattern, resulting in different colors and intensities of light.

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