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

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Ray 2 and Ray 5 are primarily considered in thin glass interference due to their stronger contributions to the interference pattern, as higher-order reflections like Ray 4 are significantly dimmer and less impactful. Each reflection diminishes in intensity, making the first-order interference the most prominent. The phase shift between Ray 2 and Ray 5 is equivalent to that of Ray 5A, ensuring constructive interference under certain conditions. However, for angles causing negative interference, secondary reflections can counteract the primary waves, leading to weaker overall contributions. This discussion highlights the importance of considering the diminishing power of secondary reflections in interference patterns.
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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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