Solve Double Slit Maxima with 3 Narrow Slits

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SUMMARY

The discussion centers on the interference pattern produced by three narrow slits with specific spacing, illuminated by monochromatic light with a wavelength of 2d/5. The introduction of a half-phase change by a filter on the bottom slit alters the expected interference outcomes. The key conclusion is that the maxima occur at sin(theta) = 6/15, as the phase change allows for constructive interference despite the destructive interference typically expected from the bottom slit. This demonstrates the importance of phase shifts in interference patterns.

PREREQUISITES
  • Understanding of wave interference principles, specifically constructive and destructive interference.
  • Familiarity with the double-slit experiment and its mathematical formulations.
  • Knowledge of phase changes in wave mechanics.
  • Ability to apply trigonometric functions to physical scenarios involving waves.
NEXT STEPS
  • Study the effects of phase shifts on interference patterns in multi-slit experiments.
  • Learn about the mathematical derivation of interference conditions for three-slit setups.
  • Explore the application of the principle of superposition in wave mechanics.
  • Investigate the role of filters in optical experiments and their impact on wave behavior.
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Students and educators in physics, particularly those focusing on wave optics and interference phenomena, as well as researchers exploring advanced optical systems.

frostchaos123
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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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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.
 

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