Deriving Snell's Law

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SUMMARY

This discussion focuses on the derivation of Snell's Law, specifically addressing the use of perpendiculars to compare two paths and the implications of angle approximations. It is established that the error associated with using perpendiculars is of higher order than first order, making this approximation valid. The angles ε and φ are discussed, with φ being shown to differ from θ₂ to first order as X approaches C, while maintaining accuracy in the distance XF through zeroth order approximation.

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  • Knowledge of first-order and higher-order approximations in calculus
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WheatNeat
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TL;DR
Why are perpendiculars used to compare the two paths, and where does this angle approximation come from?
Here we are deriving snell's law. The text compares the length of the two paths (which are assumed to be close enough such that the time difference is negligible), and uses the perpendicular to compare them. They should technically be making an isoceles triangle to compare them right? Is this an approximation? Also the text says that angle FCX is approximately equal to angle BCN', but this doesn't seem to be true in the limit as X approaches C. What am I missing?

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WheatNeat said:
TL;DR Summary: Why are perpendiculars used to compare the two paths, and where does this angle approximation come from?

Here we are deriving snell's law. The text compares the length of the two paths (which are assumed to be close enough such that the time difference is negligible), and uses the perpendicular to compare them. They should technically be making an isoceles triangle to compare them right? Is this an approximation?
Yes, that's right. You can show that the error associated with this approximation is of order higher than first order. So, it's ok.

WheatNeat said:
Also the text says that angle FCX is approximately equal to angle BCN', but this doesn't seem to be true in the limit as X approaches C. What am I missing?

Label the angles as shown.
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The angle ε is small of first order when distance XC is small compared to distance CB.

Show that ##\phi = \theta_2 + \varepsilon##. So, as X approaches C, ##\phi## differs from ##\theta_2## to first order. However, you are interested in the distance ##XF##, which equals ##XC \sin \phi##. Since ##XC## is already a small, first order quantity, ##XC\sin \phi## will be accurate to first order if you use the "zeroth order" approximation ##\phi \approx \theta_2##.
 
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