Relationship of slit, wavelength, and intensity

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Homework Help Overview

The discussion revolves around the relationship between slit width, wavelength, and intensity in the context of diffraction patterns produced by coherent electromagnetic radiation. The original poster is examining a scenario involving a slit width of 0.01 mm and various wavelengths of light, seeking to understand conditions under which intensity minima occur in the diffraction pattern.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to clarify the meaning of the diffraction pattern and whether it refers to the central maximum or the entire pattern. They express uncertainty about the implications of the slit width being less than the wavelength and its effect on intensity minima.
  • Some participants question how to visualize the diffraction pattern and the significance of the equations when the angle does not yield real solutions.
  • Others suggest considering the implications of the relationship between slit width and wavelength, particularly in terms of the existence of distinct minima.

Discussion Status

The discussion is exploring the implications of the slit width being less than the wavelength, with participants providing guidance on the breakdown of equations and the resulting absence of distinct minima in the diffraction pattern. There is an acknowledgment of the complexity of visualizing the pattern and the nature of intensity variations.

Contextual Notes

Participants are navigating assumptions about the behavior of light in diffraction scenarios, particularly the conditions under which intensity can reach zero. The original poster is also grappling with the definitions and implications of the terms used in the problem statement.

nso09
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Homework Statement


Coherent electromagnetic radiation is sent through a slit of width 0.01 mm. For which of
the following wavelengths will there be no points in the diffraction pattern where the intensity is zero?
A. Blue light of wavelength ##\lambda=500 nm##

B. Infrared light of wavelength ##\lambda=10.6 μm##

C. Ultraviolet light of wavelength ##\lambda=50 nm.##
##d=.01mm##

Homework Equations


##dsin\theta=m\lambda##
##dsin\theta=(m+.5)\lambda##

The Attempt at a Solution


I'm not sure exactly what the question is asking. What does it mean diffraction pattern? Is it just talking about the central maximum or the rest of the pattern where there are maxima and minima?
I assume this is a single slit so the minima would be where intensity is 0 so an equation that makes sense is ##dsin\theta=m\lambda##
I checked the solutions though and it said that
"If the slit width d is less than the wavelength, there are no points at the diffraction pattern at which the
intensity is zero." What does it mean that there are no points at the pattern where the intensity is 0? And why does d have to be less than the wavelength?
 
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Take your relevant equations and move the 'd' to the right hand side of them (so that the relationship between d and λ is clear). What does d being less than λ imply?
 
If d is less than ##\lambda##, then ##sin\theta\geq1##. So the domain doesn't fit ##sin\theta.## But how can I make use of the intensity since I don't have an angle to plug in ##I##=##I_0####((sin(\beta/2)/(\beta/2)##)^2 and set it equal to 0. Or is that the whole point? I don't have an angle so therefore, there are no points where intensity is 0? If so, what pattern are we talking about? The central maxima? I just need help visualizing what this whole pattern looks like.
 
Sorry for the delay in responding.

You've got the right idea. When the equations break down because there is no real solution for the angle then there will be no distinct minima. There may be a graduated continuum, but no locations where the intensity falls to zero.
 
gneill said:
Sorry for the delay in responding.

You've got the right idea. When the equations break down because there is no real solution for the angle then there will be no distinct minima. There may be a graduated continuum, but no locations where the intensity falls to zero.
Oh I see. So basically there is no point in the diffraction pattern where intensity is 0. The smallest intensity may be really tiny but never 0, therefore no waves will completely destructively interfere. Is that it?
 
Yes. That's it. The diffraction pattern disappears when d < λ.
 
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