Light Diffraction: Is Wavelength Affected by Slit Width?

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Discussion Overview

The discussion revolves around the relationship between slit width and wavelength in the context of light diffraction patterns, specifically addressing whether a slit only allows certain wavelengths based on its width. Participants explore the implications of the diffraction equation and the behavior of light through single slits.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant states that the equation sinθd = mλ/a suggests that a slit only allows certain wavelengths, questioning the influence of slit width on this phenomenon.
  • Another participant argues that single slit diffraction results in a continuum of intensity rather than specific wavelengths, challenging the initial claim about slit width restrictions.
  • A later reply emphasizes the variability of θd and its dependence on the angle of light incidence, suggesting that the original interpretation may be flawed.
  • One participant expresses confusion about the derivation of the equation and requests clarification on its origins.
  • Another participant points out that for a < λ, the equation does not yield solutions, indicating a potential misunderstanding of the conditions for proper diffraction.

Areas of Agreement / Disagreement

Participants do not reach a consensus, as there are multiple competing views regarding the relationship between slit width and wavelength, and the implications of the diffraction equation remain contested.

Contextual Notes

There are unresolved questions regarding the assumptions behind the diffraction equation and the conditions under which it applies, particularly concerning the relationship between slit width and wavelength.

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 [itex]\theta_d[/itex] were constant. But it's not. It varies from 0 to 90 degrees, with [itex]\sin \theta_d[/itex] 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 [itex]\theta_d[/itex] fits in.

For given values of [itex]\lambda[/itex] and a, different values of m give you different values of [itex]\theta_d[/itex], 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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