Understanding Interference in Thin Glass: The Role of Ray 2 and 5 Explained

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SUMMARY

This discussion focuses on the interference patterns observed in thin glass, specifically analyzing the roles of rays 2 and 5. Rays 2 and 5 are highlighted due to their significant contributions to constructive interference, while higher-order reflections, such as ray 4, are deemed less relevant due to their diminished intensity and phase shifts. The discussion emphasizes that secondary reflections, like those from ray 4, contribute minimally to the overall interference pattern, with power levels dropping significantly after each reflection due to the standard Fresnel reflection coefficients.

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As shown in the diagram , why only ray 2 and 5 are considered? When ray 4 strikes the top interface from underneath, some is reflected. Why this ray is not considered?
 
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Of course, you may calculate higher orders (4 reflects, then travels parallel to 3 - call it 3A, then 3A reflects from bottom surface, making 4A ray, which then refracts to 5A).

Two issues:
1. every such reflection is much dimmer, than previous ones. So the interference pattern from the first order is the most visible;
2. phase shift 5-5A is exactly the same, as as 2-5. Constructive interference occurs when 2-5 phase shift is n*2π. For 5A you'll have 2*n*2π - still positive interference. But - to be honest - this argument works only for positive intereference! For the angles exhibiting negative interference, every second reflection acts opposite.
 
Secondary reflections are typically quite weak. Standard Fresnel reflections from air/glass for example is about 4-5% in power. The secondary reflections are then at most (0.05)^2 - 0.25% of the original wave. Subsequent reflections rapidly drop off in power.

Claude.
 

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