Bragg's Law Experiment: Questions and Answers

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Discussion Overview

The discussion revolves around Bragg's Law and its implications in the context of diffraction phenomena, particularly in relation to x-ray diffraction in crystal lattices. Participants seek clarification on the conditions necessary for observable diffraction, the nature of wave interactions in crystals, and the theoretical versus experimental foundations of Bragg's Law.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why the wavelength of the incident wave must be comparable to the characteristic length of the system for diffraction to be evident, seeking a brief explanation related to electromagnetic fields.
  • Another participant explains that the crystal lattice acts as a diffraction grating and that constructive interference occurs when the path difference is a multiple of the wavelength, although they acknowledge their lack of expertise.
  • A participant expresses understanding of the origin of Bragg's formula but remains uncertain about specific points related to the nature of diffraction and reflection in crystals.
  • One participant asks whether the conclusion that reflection can be modeled by parallel planes in the lattice is based on experimental evidence or theoretical calculations.
  • Another participant raises a question about the nature of light in this context, suggesting that it should not be considered as a single fine line but rather in terms of probabilities.
  • Further clarification is sought regarding why certain conditions lead to observable diffraction patterns, with references to specific examples and images.

Areas of Agreement / Disagreement

Participants express varying degrees of understanding and confusion regarding the concepts discussed. There is no consensus on the specific questions raised, and multiple viewpoints exist regarding the interpretation of diffraction phenomena and the application of Bragg's Law.

Contextual Notes

Some participants note limitations in their understanding of optics compared to electromagnetic fields, which may affect their interpretations of the phenomena discussed. Additionally, there are unresolved questions regarding the relationship between theoretical models and experimental observations.

chimay
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Hi,

I read the quite common introduction to the Bragg's Law, but there are some points I have not clear at all; I hope you can help me.

1) The book says that, for the diffraction to be evident, the wave length of the incident wave must be comparable with the order of magnitude of the characteristic lenght of the system that is used for the experiment. Why is this so evident? I have no background in optics but just in EM fields, so if the answer is there, could you please explain it to me in few words?

2) Actually the problem it's far more complicated, since each atom absorbs radiation and then emits it isotropically; anyway, the experiment can be summarized by the well know formula, which models the phenomenon like the reflection of a plane wave that incides on all the planes that can be identified inside the lattice of the crystal. Does this conclusion come from experimental fact, right?

3) With reference to point 2: the formula refers two just a couple of plans, and says n \lambda = 2d\sin(\alpha)
Since the rays reflected by the cristal are parallel ( so they don't meet ), how can they give rise to constructice interference?

Thank you for any suggestion
 
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I try to explain it. In the case of x-rays the crystal lattice works as a diffraction grating.
If you want to observe constructive interference, the difference of path 2dsin(α) between two wave which are reflected by two parallele plains must be a multiple of their wavelength; so the two waves are in phase and the intensity on a radiographic screen increases. The word evident means that the phenomenon is observable.
Therefore the rule is that the two waves keep this difference of path after the reflection and so the same phase.

I'm not an expert but I hope to give you a right suggestion; however let's wait for other answers with sharp terms.
 
Thank you for your answer.
Actually I know where the Bragg's formula comes from; my doubts are explained in those 3 very specific point.
Anyway thank you!
 
chimay said:
Hi,

I read the quite common introduction to the Bragg's Law, but there are some points I have not clear at all; I hope you can help me.

1) The book says that, for the diffraction to be evident, the wave length of the incident wave must be comparable with the order of magnitude of the characteristic lenght of the system that is used for the experiment. Why is this so evident? I have no background in optics but just in EM fields, so if the answer is there, could you please explain it to me in few words?

2) Actually the problem it's far more complicated, since each atom absorbs radiation and then emits it isotropically; anyway, the experiment can be summarized by the well know formula, which models the phenomenon like the reflection of a plane wave that incides on all the planes that can be identified inside the lattice of the crystal. Does this conclusion come from experimental fact, right?

3) With reference to point 2: the formula refers two just a couple of plans, and says n \lambda = 2d\sin(\alpha)
Since the rays reflected by the cristal are parallel ( so they don't meet ), how can they give rise to constructice interference?

Thank you for any suggestion

I am not sure if I understand your questions well, but I'll try.
1). You may refer to this question: why does wavelength affect diffraction
http://physics.stackexchange.com/questions/125903/why-does-wavelength-affect-diffraction

2). Can't understand the question well. However the lights diffracted are not emitted by the atoms, but reflected. Absorption of lights by atoms need meet wavelength condition to happen.

3). I think you can't consider the light as a single fine line here but it's a probability case.

Sorry for my English.
 
1) Thank you for the link; I have read almost all the answers, but the point was different from mine. People have tried to explain why the diffraction pattern depends on the wave length by intuitive arguments. Actually, my question is the last one you can find, that is:
"The question "why does the wavelength affect diffraction", I think, could be best answered by looking at the two extreme cases. Assuming a narrow opening is illuminated..."
What I want to know is why in the first picture we don't see diffraction, while in the second we do. (please refers to the photos of the guy I have quoted )
2) I try to be more clear: Does the fact that we can study reflection by means of parallel planes of the lattice come from experimental evidence or theoretical calculations?
3) Here I don't get you answer; if we study the phenomenon by means of reflection of a plane wave with the planes of the lattice, Why can't I consider each beam like a fine line?

Thank you very very much
 

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