Light Diffraction: Is Wavelength Affected by Slit Width?

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SUMMARY

The discussion centers on the relationship between slit width and wavelength in single-slit diffraction, specifically through the equation sinθd = mλ/a, where 'a' is the slit width and 'm' represents integers excluding zero. It is established that a slit allows certain wavelengths to pass based on its width, with the diffraction pattern characterized by a continuum of intensity described by I(theta) = I0 sinc²(a sin(theta)/ λ). The participants clarify that for a < λ, the equation does not yield valid solutions, while a > λ provides proper diffraction patterns, highlighting the importance of slit dimensions relative to the wavelength.

PREREQUISITES
  • Understanding of single-slit diffraction principles
  • Familiarity with the equation sinθd = mλ/a
  • Knowledge of intensity distribution in wave optics
  • Basic grasp of the sinc function and its applications
NEXT STEPS
  • Study the derivation of the single-slit diffraction equation sinθd = mλ/a
  • Explore the concept of Fraunhofer diffraction in optics
  • Investigate the behavior of light through various slit widths and their effects on diffraction patterns
  • Examine the sinc function and its role in wave interference and diffraction
USEFUL FOR

Physics students, optical engineers, and anyone interested in wave optics and the principles of diffraction.

Gear300
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For diffraction patterns, the simple relation for the angle corresponding to dark fringes is sinθd = mλ/a, in which a is the width of the slit and m = {all integers excluding 0}. From this, it appears that a slit only allows certain wavelengths (a slit width corresponding to a length equal to an integer multiple of the wavelength). Is this true...and if so...why (the direction of propagation of the wave is perpendicular to the slit, so how would the width of the slit have such an influence)?
 
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I don't know where you get this from, or I misunderstand your question.

If you send light on a single slit, then you get a an outgoing light distribution with a continuously varying intensity as a function of the angle

The diffraction by a single slit is different. It doesn't give you specific Bragg angles, but a specific continuum of intensity as a function of angle given by a formula of the kind:

I(theta) = I0 sinc^2(a sin(theta)/ lambda)

(or something of the kind, I didn't check).

Now, that's a function with zeros at specific angles, and those angles are given by the formula you stated. Note that m=0 is not a solution: the direct beam always gets through (eh, as you noted yourself).

What makes you think that no light of an arbitrary wavelength can get through ?
 
Gear300 said:
For diffraction patterns, the simple relation for the angle corresponding to dark fringes is sinθd = mλ/a, in which a is the width of the slit and m = {all integers excluding 0}. From this, it appears that a slit only allows certain wavelengths (a slit width corresponding to a length equal to an integer multiple of the wavelength). Is this true...and if so...why (the direction of propagation of the wave is perpendicular to the slit, so how would the width of the slit have such an influence)?

Er... try doing this with an incandescent light bulb and then look at the resulting diffraction. You'll see for yourself how what you see falsifies what you think here.

Zz.
 
Gear300 said:
it appears that a slit only allows certain wavelengths (a slit width corresponding to a length equal to an integer multiple of the wavelength).

This would be true if \theta_d were constant. But it's not. It varies from 0 to 90 degrees, with \sin \theta_d varying correspondingly from 0 to 1, depending on the position the light arrives at your viewing screen. The source where you got that equation should have a diagram showing the geometry of the situation and how \theta_d fits in.

For given values of \lambda and a, different values of m give you different values of \theta_d, which give you the positions on the screen at which the diffracted light is at a minimum.
 
Looks like I misunderstood the content. But, I'm still not understanding how the equation came up. Could anyone go ahead and post a proper derivation of the equation sinθd = mλ/a??
 
Look up single slit diffraction (Fraunhofer diffraction) in any textbook. Or try this: http://hyperphysics.phy-astr.gsu.edu/hbase/phyopt/sinslit.html"
 
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Thanks...I looked into it more...

I think I found the source of my misunderstanding. For a*sinθd = mλ, if a < λ, θd does not have a solution within a single domain, whereas a > λ would hold proper solutions. Earlier in the text, it was stated that (or I read it as) proper diffraction occurs for slits comparable to or smaller than the wavelength, which seems to contradict the equation above.
 

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