Solve Double Slit Maxima with 3 Narrow Slits

In summary, when a filter is introduced on the bottom slit of a system with 3 narrow slits, irradiated by monochromatic light with a wavelength of 2d/5, the resulting interference pattern will have a maximum at sin(theta) = 6/15 due to the constructive interference of the waves from the middle and bottom slits. The extra phase change introduced by the filter cancels out part of the phase difference, allowing for this maximum to occur.
  • #1
frostchaos123
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0

Homework Statement



3 narrow slits with spacing of d and 3d/2 as in picture, the slits are irradiated from left with a plane of monochromatic light with wavelength 2d/5.

If the bottom slit is covered with a filter that introduces a half phase change, how many
principal maxima will be observed?

5l17px.png


Homework Equations



2 slit constructive interference: d sin(theta)= m * wavelength
destructive interference: d sin(theta) = (m + 0.5) * wavelength



The Attempt at a Solution



The top slit has constructive intereference of d * sin(theta) = m * (2d/5), which gives
sin(theta) = 0, 2/5, 4/5 for m = 0,1,2,...

The bottom slit has destructive intereference of 3d/2 * sin(theta) = (m+1/2) * (2d/5), which gives
sin(theta) = 2/15, 6/15, 10/15, ... for m = 0,1,2,...

My question is that the answer given is that sin(theta) = 6/15 will be the maxima, since it occurs at for both top and bottom slit, but why is it so?

Shouldn't the destructive interference of the bottom slit cancel out the constructive interference at sin(theta) = 6/15, making it not the maximum?

Thanks.
 
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  • #2
frostchaos123 said:

Homework Statement



3 narrow slits with spacing of d and 3d/2 as in picture, the slits are irradiated from left with a plane of monochromatic light with wavelength 2d/5.

If the bottom slit is covered with a filter that introduces a half phase change, how many
principal maxima will be observed?

5l17px.png


Homework Equations



2 slit constructive interference: d sin(theta)= m * wavelength
destructive interference: d sin(theta) = (m + 0.5) * wavelength



The Attempt at a Solution



The top slit has constructive intereference of d * sin(theta) = m * (2d/5), which gives
sin(theta) = 0, 2/5, 4/5 for m = 0,1,2,...

The bottom slit has destructive intereference of 3d/2 * sin(theta) = (m+1/2) * (2d/5), which gives
sin(theta) = 2/15, 6/15, 10/15, ... for m = 0,1,2,...
This would be true if no filter were present in front of the bottom slit. The extra phase change the filter introduces cancels part of the phase difference due to the difference in path length, so the waves from the middle and bottom slits constructively interfere when this condition holds.
My question is that the answer given is that sin(theta) = 6/15 will be the maxima, since it occurs at for both top and bottom slit, but why is it so?

Shouldn't the destructive interference of the bottom slit cancel out the constructive interference at sin(theta) = 6/15, making it not the maximum?

Thanks.
 

1. What is the double slit experiment?

The double slit experiment is a classic experiment in physics that demonstrates the wave-particle duality of light. It involves shining a beam of light through two parallel slits and observing the resulting interference pattern on a screen behind the slits.

2. What is the significance of adding a third narrow slit?

The addition of a third narrow slit in the double slit experiment allows for more complex interference patterns to be observed. It also allows for the study of multi-slit interference, which has important applications in optics and quantum mechanics.

3. Why are there multiple maxima in the resulting interference pattern?

The multiple maxima in the interference pattern are a result of the constructive and destructive interference of light waves passing through the slits. This is due to the different path lengths and phases of the waves as they pass through the slits.

4. How does the spacing of the slits affect the interference pattern?

The spacing of the slits directly affects the spacing of the maxima in the interference pattern. As the distance between the slits increases, the spacing between the maxima also increases. This can be seen in the mathematical formula for the double slit interference pattern: d sinθ = mλ, where d is the slit spacing, θ is the angle of diffraction, m is the order of the maximum, and λ is the wavelength of the light.

5. What are the practical applications of studying the double slit experiment with 3 narrow slits?

Studying the double slit experiment with 3 narrow slits has practical applications in various fields, including optics, quantum mechanics, and telecommunications. It allows for the manipulation and control of light waves, which is essential in technologies such as lasers, fiber optics, and holography. It also provides insights into the behavior of particles at the quantum level, leading to advancements in quantum computing and cryptography.

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